KR101089435B1 - Micro-optic security and image presentation system - Google Patents

Abstract

The present invention provides a film that uses a regular two-dimensional array of non-cylindrical lenses to magnify a micro-picture called an icon and to form a composite enlarged image through the integrated capabilities of multiple individual lens / icon picture systems. It is about the material. A composite magnification micro-optical system is formed of a periodic planar array of one or more optical spacers 5, a plurality of image icons 4 having an axis of symmetry with respect to at least one of its planar axes and on or on the optical spacers 5. A periodic planar array of image icon focusing elements 1 having a micro-picture arranged adjacently, and an axis of symmetry with respect to at least one of its plane axes, the axis of symmetry being the same plane axis as that of the micro-picture plane array 4. The system of the present invention can provide a number of individual visual effects, such as three-dimensional and motion effects.

Optical spacer, image icon, focusing element, F number, parallax motion, effective diameter, focal length, morphing effect, reflective layer

Description

MICRO-OPTIC SECURITY AND IMAGE PRESENTATION SYSTEM

Related application

This application is directed to US Provisional Application No. 60 / 524,281, filed November 21, 2003, US Provisional Application No. 60 / 538,392, filed January 22, 2004, and 2004, each of which is incorporated herein in its entirety. Claims and claims priority to U.S. Provisional Application No. 60 / 627,234, filed November 12, date.

The present invention relates to a synthetic magnification micro-optical system formed as a polymer film in an exemplary embodiment. The special optical effects provided by the various embodiments herein can be used as security devices for clear and confidential authentication of bills, documents, and products as well as visual enhancement of products, packaging, printed materials, and consumer goods.

Various optical materials have been used to provide certification of bills and documents, to verify authenticity and to identify from counterfeits, and to provide visual reinforcement of manufactured articles and packaging. Examples include holographic displays, and other imaging systems including lens structures and arrays of spherical micro-lenses. Holographic displays have been widely used in credit cards, driver's licenses, and clothing tags.

An example of a lenticular structure for document security is disclosed in US Pat. No. 4,892,336 to Kaule et al., Which relates to a security security thread to be embedded in a document to provide anti-counterfeiting means. A security hidden line is a transparent body having a printing pattern on one side and a lens lens structure that cooperates with the printing pattern on the other side. The lens lens structure is described as consisting of multiple parallel cylindrical lenses or alternatively as spherical or honeycomb lenses.

U. S. Patent No. 5,712, 731 to Drinkwater et al. Discloses a security device having an array of micro-pictures associated with an array of nearly spherical micro-lenses. This lens may also be an astigmatism lens. Each lens is usually 50 to 250 mu m, and usually has a focal length of 200 mu m.

Both of these approaches have similar drawbacks. The result is a relatively thick structure, which is not particularly suitable for use in document authentication. The use of cylindrical or spherical lenses provides a narrow field of view and therefore blurs the image, and the focus of the lens requires accurate and difficult alignment with the associated image. In addition, it has not proven particularly effective as a security or anti-counterfeiting measure.

Given the above and other shortcomings, the present invention provides a secure and visually unique optical material capable of promoting clear certification of banknotes, documents, articles of manufacture, and products, and optical materials that provide visual reinforcement of articles of manufacture, products, and packaging. There is a demand in the industry.

The present invention uses a regular two-dimensional array of non-cylindrical lenses to magnify micro-pictures, referred to herein as icons, and to form composite enlarged images through the integrated capabilities of multiple individual lens / icon imaging systems. It relates to the film material to make. The composite enlarged image and the background surrounding it may be colorless or colored, and either or both of the image and the background surrounding it may be transparent, translucent, colored, fluorescent, phosphorescent, display optically variable color, metallized, or It can be almost retroreflective. Materials displaying color images on a transparent or colored background are particularly suitable for use in combination with the underlying printed information. When one such material is applied onto the printed information, both the printed information and the image are seen simultaneously in a three-dimensional or dynamic motion relationship with each other. This kind of material can also be overprinted, i.e. have a print applied to the top (lens) surface of the material. Alternatively, materials displaying color images (of any color, including black and white colors) on translucent or almost opaque backgrounds of different colors are particularly suitable for use alone or overprinted without being combined with the underlying print information. Ideal for use with information.

The degree of composite magnification achieved can be controlled by selecting several factors including the degree of 'skew' between the axis of symmetry of the lens array and the axis of symmetry of the icon array. A regular periodic array has an axis of symmetry whose magnitude is infinite in an ideal array, which defines the lines that the pattern can be reflected around without changing the pattern's basic shape. If the sides of the rectangle are aligned with the x- and y-axes of the plane, for example, the sides of the rectangle can be reflected around any diagonal of any rectangle without changing the relative orientation of the array, the sides of the rectangle become all sides. If they are identical and indistinguishable they will still be aligned with the post-reflection axis.

Instead of mirroring the rectangular array, the array can be rotated by an angle equal to the angle between the axes of symmetry of the same type. In the case of a rectangular array, the array can be rotated by an angle of 90 degrees, the angle between the diagonals, to reach an array orientation that is indistinguishable from the original array. Similarly, a regular array of hexagons includes a number of hexagons, including a "diagonal line" (a line connecting two opposite vertices) or a "point divider line" (a line connecting the center points of faces on opposite sides of the hexagon). It can be mirrored or rotated about its axis of symmetry. The angle between the symmetry axes of either type is 60 degrees, resulting in an array orientation that is indistinguishable from the original orientation.

If the lens array and icon array are initially arranged such that their planar dimensions form their respective xy planes, one axis of symmetry is selected to represent the x-axis of the first array, and the corresponding shape to represent the x-axis of the second array. The axis of symmetry (e.g., the diagonal axis of symmetry) is chosen, and the two arrays are separated by a nearly uniform distance in the z-axis direction, and these arrays show zero slope if the x-axis of the array looks parallel to each other in the z-axis direction. Say you have it. If one array rotates at an angle of 60 degrees or multiples in the case of a hexagonal array, then the hexagonal array is again aligned with no inclination as if there was no slope during rotation of 90 degrees or multiples of the square array. Any angular misalignment between x-axes that is distinct from this "zero oblique rotation" is referred to as oblique. Small slopes, such as 0.06 degrees, can produce large magnifications above 1,000x, and large slopes, such as 20 degrees, produce small magnifications, such as 1x. Other factors, such as the relative scale of the two arrays and the F # of the lens, can affect the magnification of the composite image as well as its rotation, orthoparallactic motion, and apparent visual depth.

A number of apparent visual effects that may be provided by the materials of the present invention (hereinafter generally referred to as "unison" for materials or their respective "Unison Motion", "unison" for Unison materials "Unison Deep", "Unison SuperDeep", "Unison Float", "Unison Levitate", "Unison Morph", and "Unison 3-D There are a number of distinct visual effects referred to as ", and various embodiments thereof produce each of the effects as described below:

Unison motion represents an image showing an orthoparallactic movement (OPM), and when the material is inclined, the image moves in an oblique direction that looks perpendicular to the direction expected by the parallax. Unison Dips and Super Dips represent images that visually appear to lie in a space plane deeper than the thickness of the material. Unison floats and superfloats represent images that appear to lie in a space plane at a distance above the surface of the material; Unison flotation swings from a Unison Dip (or Superfloat) to a Unien float (or SuperFloat) when the material is rotated by a given angle (eg, 90 degrees), and then again when the material rotates the same angle further Super Dip). Unison morphs represent a composite image that changes shape, shape, or size when the material is rotated or viewed from another perspective. Unison 3-D represents an image showing a large three-dimensional structure, such as a facial image.

Multiple unison effects may be combined in one film, such as a film comprising a plurality of unison motion picture planes that may differ in shape, color, direction of movement, and magnification. Other films can combine unison deep image planes and unix float image planes, while other films can be designed to combine unison deep, unison motion, and unison float layers in the same or different colors, and these images are the same Or have different graphical elements. The colors, graphic designs, optical effects, magnifications, and other visual elements of multiple image planes are often independent, with the exception of which the planes of these visual elements can be combined in any manner.

For many bills, documents, and product security applications, the overall thickness of the film is less than 50 microns (also referred to herein as "μ" or "μm"), for example less than approximately 45 microns, and in further examples, approximately 10 microns. It is preferably in the range of from about 40 microns. This can be achieved, for example, by using a focusing element having an effective base diameter of less than 50 microns, in another example less than 30 microns, and in another example approximately 10 microns to 30 microns. As another example, a focusing element can be used having a focal length of less than approximately 40 microns, in further examples a focal length of approximately 10 to approximately 30 microns. In a particular example a focusing element with a base diameter of 35 microns and a focal length of 30 microns can be used. Alternative hybrid refraction / reflection examples can be made thin as 8 microns.

The film herein is excellent in anti-counterfeiting due to its complex multilayer structure and its high aspect-ratio elements, which are difficult to reproduce by conventional manufacturing systems.

Accordingly, the system of the present invention provides a micro-optic system in the form of a polymer film having a thickness that projects one or more images as seen by the naked eye with reflected or transmitted light:

i. Show parallax motion (unison motion);

Ii. Appear to lie on a space plane deeper than the thickness of the polymer film (unison dip and unison super dip);

Iii. Appear to lie on the surface of the polymer film on the space plane (union float and unison superfloat);

Iii. When the polymer film is azimuth rotated, it swings between a space plane deeper than the thickness of the polymer film and a space plane higher than the surface of the film (unison flotation);

v. Transform from one shape, shape, size, color (or any combination of these properties) to another shape, shape, size, color (or any combination of these properties) (unison morph); And / or

Iii. It appears to have realistic three-dimensionality (Union 3-D).

More specifically, the present invention,

(a) one or more optical spacers,

(b) a micro image consisting of a periodic planar array of a plurality of image icons having an axis of symmetry about at least one of the plane axes, disposed on or adjacent to the optical spacer, and

(c) a periodic planar array of image icon focusing elements having an axis of symmetry about at least one of the plane axes, wherein the axis of symmetry is the same plane axis as that of the micro image plane array, each focusing element being a polygonal base multi-region focusing element Or a lens that provides an enlarged field of view relative to the width of the associated image icon so that the peripheral edge of the associated image icon does not leave the field of view, or an aspheric focusing element having an effective diameter of less than 50 microns. A synthetic augmented micro-optical system comprising a periodic planar array of icon focusing elements, and a method of manufacturing the same.

The system of the present invention may have one or more of the above effects. A method is provided for selectively including the above effects in the present system.

The invention further relates to or in secure documents, labels, tear strips, tamper resistant devices, sealing devices, or other authentication or security devices, including at least one micro-optical system described above. A security device is provided that is at least partially included and suitable for use on or in connection with it. More specifically, the present invention,

(a) one or more optical spacers,

(b) a micro image consisting of a periodic planar array of a plurality of image icons having an axis of symmetry about at least one of the plane axes, disposed on or adjacent to the optical spacer, and

(c) a periodic planar array of image icon focusing elements having an axis of symmetry about at least one of the plane axes, wherein the axis of symmetry is the same plane axis as that of the micro image plane array, each focusing element being a polygonal base multi-region focusing element A periodic plane of the image icon focusing element, or a lens that provides an enlarged field of view relative to the width of the associated image icon so that the peripheral edge of the associated image icon does not leave the field of view, or an aspherical focusing element having an effective diameter of less than 50 microns. A document security device comprising an array, and a method of manufacturing the same.

In addition, the present invention provides the effects described above for the visual enhancement of apparel, skin products, documents, printed materials, goods, packaging, point of sale information displays, publications, advertising devices, sporting goods, financial documents and trading cards, and all other products. Provided is a visual enhancement device comprising at least one micro-optical system described above.

In addition, a security document or label is provided wherein at least one security device described above is at least partially embedded therein and / or thereon.

Other features and advantages of the invention will be apparent to those skilled in the art from the following detailed description and the accompanying drawings.

Other systems, devices, methods, features, and advantages will become apparent to those skilled in the art upon examination of the following detailed description and drawings. It is to be understood that all such additional systems, methods, features, and advantages are included herein, are included in the scope of the present invention, and are protected by the claims.

Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art. All publications, patent applications, patents, and other references mentioned herein are incorporated by reference in their entirety. In case of conflict, the present specification, including definitions, will control. In addition, the materials, methods, and examples are illustrative only and should not be construed as limiting.

Various aspects of the invention may be better understood by referring to the drawings. The parts in the figures are not necessarily drawn to scale, and may be highlighted to clarify the principles of the invention. Moreover, like reference numerals designate like parts in the various drawings.

1A is a cross-sectional view of a micro-optical system illustrating one embodiment of the present invention for providing parallax motion of an image of a system.

1B is an isometric cutaway view of the embodiment of FIG. 1A.

FIG. 2A illustrates the four-way parallax composite image motion effect of the embodiment of FIGS. 1A-B.

2b-c illustrate the visual effects of the dip and float embodiments of the present system.

2d-f illustrate the visual effects obtained by the rotation of the lift embodiment of the present system.

3A-I are plan views illustrating various embodiments and fill rates of different patterns of symmetrical two-dimensional arrays of lenses of the present system.

4 is a graph showing the different combinations of dip, union, float, and flotation embodiment effects generated by a change in the icon element period / lens period ratio.

5A-C are plan views showing how the composite enlargement of the icon image can be controlled by the relative angle between the lens array axis and the icon array axis of the present system.

6A-C are plan views showing an embodiment of achieving the morphing effect of the composite enlarged image of the present system.

7A-C are cross-sectional views illustrating various embodiments of the icon layer of the present system.

8A-B are plan views illustrating embodiments of 'positive' and 'negative' icon elements.

Fig. 9 is a cross-sectional view showing one embodiment of a multi-level material for generating regions having different characteristics in a composite enlarged image.

Fig. 10 is a cross-sectional view showing another embodiment of a multi-level material for producing regions having different characteristics in a composite enlarged image.

11A-B are cross-sectional views showing reflective and pinhole optical embodiments of the present system.

12A-B are cross-sectional views comparing the structure of a pre-refractive material embodiment with a hybrid refractory / reflective material embodiment.

Fig. 13 is a sectional view showing an embodiment of a 'peel-exposed' tamper-evident material.

14 is a cross-sectional view illustrating an embodiment of a 'peel-change' tamper resistant material.

15A-D are cross-sectional views illustrating various embodiments of a two-sided system.

16A-F are cross sectional and corresponding top views illustrating three different methods for generating a gradation or hue icon element pattern and subsequent composite enlarged image by the present system.

17A-D are cross-sectional views illustrating the use of the present system with printed information.

18A-F illustrate the application or incorporation of the present system to various substrates in combination with printed information.

19A-B are cross-sectional views comparing the focused field of view of the spherical lens with that of the plainfield aspheric lens, each of which is incorporated into the present system.

20A-C are cross-sectional views illustrating two advantages in use resulting from the use of thick icon layers in the present system.

21A-B are plan views showing that the system is applied as a " partial exposure " hidden line to banknotes.

Figure 22 illustrates a four-way parallax motion embodiment of the present system of images with "partial exposure" security hidden lines.

Figure 23 shows halftone processing of the composite image of the present system.

Figure 24A illustrates the use of the present system to produce a combined composite image of dimensions smaller than the minimum features of the individual composite images.

Fig. 24B illustrates the use of the present system for creating a narrow gap pattern between icon picture elements.

Fig. 25 illustrates the inclusion of secretly hidden information in the icon image of the present system.

Fig. 26 shows the generation of a full three-dimensional image by the present system.

FIG. 27 shows a method for designing an image icon in the three-dimensional embodiment of FIG.

FIG. 28 shows an icon image obtained from the method of FIG.

Figure 29 shows how the method of Figure 27 can be applied to a complex three-dimensional composite image.

30 shows the center region focusing characteristics of an exemplary hexagonal base multi-region lens having an effective diameter of 28 microns.

Figure 31 shows the central area focusing characteristics of a spherical lens having a diameter of 28 microns.

32 shows the performance of the side regions of the hexagonal lens of FIG.

FIG. 33 shows the performance of the outer region of the spherical lens of FIG.

The embodiment disclosed in the drawings will now be described in detail. While several embodiments have been disclosed in conjunction with these drawings, the present invention is not limited to these embodiments. Rather, the present invention is to be understood to cover all variations, modifications, and equivalents.

1A illustrates one embodiment of a micro-optical system 12 that provides parallax motion of an image of the system.

The system 12 has a micro-lens 1 having at least two substantially identical axes of symmetry and arranged in a two-dimensional periodic array. The lens diameter 2 is preferably less than 50 μ, and the interstitial space 3 between the lenses is preferably 5 μ or less (“μ” and “μm” are used alternately to mean the same measurement). . The micro-lens 1 focuses the image of the icon element 4 and projects this image 10 towards the viewer. The system is generally used in situations with a normal level of ambient light, so that the illumination of the icon image is from the reflected or transmitted ambient light. The icon element 4 is one element of a periodic array of icon elements having a period and dimensions substantially similar to the lens array comprising the lens 1. There is an optical spacer 5 between the lens 1 and the icon element 4, which may be in contact with the material of the lens 1 or optionally a separate substrate 8, in this embodiment the lens ( 9) is separated from the substrate. The icon element 4 may optionally be protected by a sealing layer 6 which is preferably made of a polymeric material. The sealing layer 6 may be transparent, translucent, tinted, pigmented, opaque, metallic, magnetic, variable, or any combination thereof, and may be optical effects, electrically conductive or capacitive, magnetic fields It provides desirable optical effects and / or additional functionality for security and authentication purposes, including support for automatic currency authentication, verification, tracking, counting, and detection systems, which rely on detection.

The overall thickness 7 of the system is usually less than 50 μ and the actual thickness is dependent on the F # (F number) of the lens 1 and the thickness of the lens 2 and the thickness of the additional security feature or visual effect layer. The repetition period 11 of the icon element 4 is almost the same as the repetition period of the lens 1, and the "scale ratio" is the ratio of the repetition period of the icon to the repetition period of the lens in order to produce various different visual effects. ) "Is used. If the axial symmetry value of the scale factor is approximately equal to 1.0000, the unison motion lag parallax effect is obtained when the symmetry axis of the lens and icon is misaligned. If the axial symmetry value of the scale factor is less than 1.0000, the axis of symmetry of the lens and icon is substantially Unison dip and Unison superdip effects are obtained when aligned, and if the axial symmetry of the scale ratio exceeds 1.0000, the Unison float and Unison superfloat effects are obtained when the symmetry axis of the lens and icon is substantially aligned. If the axial symmetry value of the scale ratio is 0.995 in the X direction and 1.005 in the Y direction, the unison flotation effect is obtained.

The unison morph effect can be obtained by scale modification of one or both of the lens repetition period and the icon repetition period, or by including spatially varying information in the icon pattern. Unison 3-D effects can also be obtained by including spatially varying information in the icon pattern, but in this embodiment the information represents different viewpoints of the three-dimensional object viewed from a particular location that closely matches the location of the icon.

FIG. 1B shows an isometric view of the system shown in cross section in FIG. 1A, with a rectangular array pattern of lenses 1 and icons 4 of repeating period 11 and optical spacer thickness 5 (FIG. Not specific to a square array pattern, but is a representative cross-sectional view of all regular periodic array patterns). Icon element 4 is shown as a "$" image as is clearly seen in the front cutaway view. Although there is a substantially one-to-one correspondence between the lens 1 and the icon element 4, the axis of symmetry of the lens array will generally not be exactly aligned with the axis of symmetry of the icon array.

In the case of the unison (quadrome motion) material embodiment of FIGS. 1A and 1B having a scale ratio of 1.0000, the resulting composite image of the icon element when the lens 1 axis and the icon element 4 axis are substantially aligned. (In this example, the huge "$") is "inflated" and expanded by a factor that theoretically approaches infinity. A slight angular misalignment of the lens 1 axis and the icon element 4 axis reduces the magnification factor of the composite image of the icon element, resulting in the rotation of the enlarged composite image.

The synthetic magnification factors of the Unison Dip, Unison Float, and Unison Flotation embodiments depend on the angular alignment of the lens 1 axis and the icon element 4 axis as well as the scale ratio of the system. When the scale ratio is not equal to 1.0000, the maximum magnification obtained from the substantial alignment of these axes is equal to the absolute value of 1 / (1.0000- (scale ratio)). Thus, a unison dip material with a scale ratio of 0.995 will exhibit a maximum magnification of | 1 / (1.000-0.995) | = 200x. As with the Unison Motion Material embodiment, slight angular misalignment of the Lens 1 axis and the Icon element 4 axis of the Unison Dip, Unison Float, and Unison Flotation embodiments reduces the magnification factor of the composite image of the icon element and enlarges it. Results in rotation of the composite image.

The composite image generated by the Unison Dip or Superdip icon pattern is perpendicular to the orientation of the Unison Dip or Superdip pattern, and the composite image generated by the Unison float or Superfloat icon pattern is the orientation of the Unison float or Superfloat icon pattern It is rotated upside down by one hundred eighty degrees (180 °).

FIG. 2A schematically illustrates the semi-intuitive, parallax picture motion effect seen in the unison motion embodiment. FIG. The left side of FIG. 2A shows a planar view of one unison motion material 12 swinging 18 around the horizontal axis 16. If the composite enlarged image 14 is moved in time, this image will appear to be displaced up and down (as shown in FIG. 2A) when the material 12 is swung around the horizontal axis 16. This apparent parallax motion will be typical of real objects, conventional prints, and holographic images. Instead of representing the parallax motion, the composite enlarged image 14 shows the parallax motion 20 which is a motion perpendicular to the normally expected parallax motion direction. The right side of FIG. 2A shows a perspective view of one material 12 representing the four-way parallax motion of a single composite enlarged image 14 when rocking 18 around the horizontal axis of rotation 16. The dotted outline 22 shows the position of the composited enlarged image 14 after moving to the right by the parallax, and the outline 24 illustrated by dotted line is synthesized after moving to the left by the parallax The position of the enlarged image 14 is shown.

The visual effects of the Unison Dip and Unison Float embodiments are shown isometric in FIGS. 2B, C. In FIG. 2B, one unison dip material 26 shows a composite enlarged image 28 that appears three-dimensionally to lie below the plane of the unison dip material 26 when viewed by the observer 30 's eye. In FIG. 2C, one unison dip material 32 shows a composite enlarged image 34 that appears three-dimensionally to lie on the plane of unison float material 34 when viewed by the observer 30 's eye. The unison dip effect and unison float effect are typically shallow shallow elevations of less than 45 degrees from the vertical altitude (so that the line of sight from the observer's 30 eyes to the unison dip material 26 or unison float material 32 is perpendicular to the surface of the material).仰角: can be seen from the omnidirectional observation position over a wide range of elevation positions up to elevation angles. The visibility of the Unison Dip and Unison float effects over a wide range of viewing angles and orientations provides a simple and convenient way to distinguish Unison dip and Unison float materials from simulation using cylindrical lens optics or holography.

The Unison flotation embodiment effect is, in FIGS. 2D-F, an isometric view showing the three-dimensionally perceived depth position of the composite enlarged image 38 in three different azimuth rotations of the Unison flotation material 36, and the observer 30. Is shown in a corresponding plan view of the visible unification floatation material 36 and the composite enlarged image 38. FIG. 2D shows a composite enlarged image 38 (hereinafter referred to as “image”) that appears three-dimensionally to lie in a plane underneath the Unison Float Material 36 when the Unison Float Material 36 is oriented as shown in plan view. To show. The dark black line in the plan view serves as the azimuth orientation reference 37 for explanation. It should be noted that in FIG. 2D the orientation reference 37 is aligned in the vertical direction and the image 38 is aligned in the horizontal direction. Since the scale ratio (hereinafter referred to as the 'stereoscopic scale ratio') is less than 1.000 along the first axis of the unison flotation material 36 aligned almost parallel to the line connecting the pupils of the observer's eyes, the image 38 is Appears at Unison Deep. The stereoscopic scale ratio of unison flotation material 36 is greater than 1.000 along a second axis perpendicular to the first axis, so that the second axis is approximately parallel to the line connecting the pupil of the observer's eye as shown in FIG. 2F. It produces the unison float effect of the image 38 when aligned. Note that the orientation reference 37 in this figure is in the horizontal position. FIG. 2E shows the intermediate orientation orientation of the Unison flotation material 36 which produces a difference motion omnidirectional image effect since the stereoscopic scale ratio in this orientation orientation is approximately 1.000.

When the material is rotated azimuthally, from underneath flotation material 36 (FIG. 2D) to the level of unison flotation material 36 (FIG. 2E) and then above the level of unison flotation material 36 (FIG. 2F). The visual effect of the moving unison flotation image 38 can be enhanced by combining the unison flotation material 36 with information printed in a conventional manner. The constant stereoscopic depth of conventional prints acts as a reference plane for better perception of stereoscopic depth shifting of the image 38.

When the unison material is illuminated by a strong directional light source, such as a 'point' light source (e.g. a spotlight or an LED flashlight) or a parallel light source (e.g. sunlight), a "shadow image" of the icon can be seen. These shadow pictures are special in many ways. The composite image provided by Unison does not move as the illumination direction moves, but the generated shadow image moves. Also, the unison composite image may lie in a different visual plane than the plane of material, while the shadow image always lies in the material plane. The color of the shadow picture is the picture of the icon. Thus, the black icon generates a black shadow image, the green icon generates a green shadow image, and the white icon generates a white shadow image.

The movement of the shadow image as the illumination angle moves is constrained to a particular depth or motion union effect to be parallel to the visual effects present in the composite image. Thus, the movement of the shadow image as the illumination angle is changed is parallel to the movement shown by the composite image when the vision is changed. Especially,

Motion shadow images move in a parallax manner when the light source moves.

The deep shadow image moves in the same direction as the light source.

The float shadow image moves in the opposite direction to the light source.

The levitation shadow image moves in the direction that is the combination of the above.

Float deep shadow images move in the same direction as light in the left and right directions but in the opposite direction to light in the up and down directions, and flotation float shadow images move in the same direction as the light in the left and right directions but in the same direction as light in the up and down directions. The levitation motion shadow image represents parallax motion with respect to light movement.

Unison morph shadow images show morphing effects as the light source moves.

Additional dichroic shadow imaging effects appear when divergent point light sources, such as LED light, are moved closer and away from the unison film. As the light source gets farther away, its divergent rays are closer to parallel light and the shadow image produced by the dip, superdeep, float or superfloat unison composite image appears to be about the same size as the composite image. As the light gets closer to the surface, the shadow image of the dip and superdeep materials is reduced because the illumination is much more divergent, and the shadow image of the float and superfloat materials is enlarged. When these materials are illuminated with converging illumination, the dip and superdeep shadow images are enlarged to a larger size than the composite image, and the float and superfloat shadow images are reduced.

When the convergence or divergence of the illumination is changed, the shadow image of the unison motion material does not change significantly in scale, but rather the shadow image rotates around the illumination center. When the convergence or divergence of the illumination changes, the Unison flotation shadow image is reduced in one direction and enlarged in the vertical direction. When the convergence or divergence of the lighting is changed, the unison morph shadow image is changed in a manner specific to the particular morph pattern.

These shadow picture effects can all be used as additional authentication methods for Unison materials used in security, anti-counterfeiting, trademark protection applications, and other similar applications.

3A-I are plan views illustrating various embodiments and fill-factors of different patterns of symmetrical two-dimensional arrays of micro-lenses. 3a, d, and g show micro-lenses 46, 52, and 60, respectively, arranged in a regular hexagonal array pattern 40. As shown in FIG. (The dotted array pattern lines 40, 42, 44 depict the symmetry of the lens pattern, but do not necessarily represent any physical element of the lens array.) The lens of FIG. 3A has a nearly circular basic geometry. 3), the lens of FIG. 3G has a substantially hexagonal base shape 60, and the lens of FIG. 3D has a rounded hexagonal intermediate base shape 52. Similar developments in lens shape apply to rectangular arrays 42 of lenses 48, 54 and 62, which are rounded rectangles 54 from nearly circular 48, as shown in Figs. ), It has a basic shape up to almost a square (62). Correspondingly, the equilateral triangle array 44 holds a lens having a basic shape ranging from almost circular 50 to rounded triangle 58 and nearly triangle 64, as shown in Figs. 3c, f and i. .

The lens pattern of Figures 3A-I represents a lens that can be used in the present system. The intergrid space between the lenses does not directly contribute to the enlargement of the synthesis of the image. The material created using one of these lens patterns will also have an array of icon elements arranged in the same shape and on approximately the same scale, to create Unison Motion, Unison Dip, Unison Float, and Unison Float effects. It will allow for differences in the scale used. As shown in Fig. 3C, when the inter-grid space is large, it is said that the lens has a low filling rate, and the contrast between the image and the background will be reduced by the light scattered from the icon element. If the inter-grid space is small, it is said that the lens has a high filling rate, and if the lens itself has good focusing characteristics and the icon element is in the focal plane of the lens, the contrast between the image and the background will be high. In general, it is easier to form high optical quality micro-lenses based on circular or near circular rather than square or triangle based. The minimization of inter-lattice spacing and a good balance of lens performance is shown in FIG. 3D, which shows a hexagonal array of lenses having a rounded hexagonal base shape.

Lenses with a low F # are particularly suitable for use in the system of the present invention. Low F # means less than 4, especially about less than 2 in unison motion. Low F # lenses have a high curvature and have a correspondingly large sag, or central thickness, as a percentage of its diameter. A typical Unison lens with an F # of 0.8 has a hexagonal base having a width of 28 microns and a center thickness of 10.9 microns. A typical Drinkwater lens having a width of 50 microns and a focal length of 200 microns has a F # of 4 and a center thickness of 3.1 microns. When scaled to the same base size, unison lenses have a deflection nearly six times larger than drink water lenses.

Polygonal base multi-domain lenses, such as, for example, hexagonal base multi-zonal lenses, have been found to have significant and surprising advantages over circular base spherical lenses. As mentioned above, hexagonal base multi-domain lenses significantly improve manufacturability due to their stress-relaxing shape, but there are additional surprising optical advantages obtained through the use of hexagonal base multi-domain lenses.

These lenses are referred to as multi-regional because they each have three optical regions that provide different and unique advantages to the present invention. These three regions are the central region (constituting almost half of the lens area), the side region, and the corner region. These polygonal lenses have an effective diameter which is drawn inside the corner area around the center area and is the diameter of the circle with the side area.

The central region of the hexagonal base multi-region lens of the present invention is not only defined for spherical surfaces having the same diameter and focal length, but also for aspherical shapes for focusing light (e.g., 28 micron diameter lenses having a nominal 28 micron focal length. y = (5.1316E) X4- (0.01679) X3 + (0.124931) X + 11.24824]. 30 illustrates the central region 780 focal characteristics 782 of a nominal 28 micron diameter hexagonal base multi-region lens 784 with a nominal 28 micron focal length on a polymer substrate 786 (lens and substrate n = 1.51). 31 shows the central region 788 focal characteristics 790 of a nominal 28 micron diameter spherical lens 792 having a nominal 30 micron focal length on a polymer substrate 794 (lens and substrate n = 1.51). Illustrated. Comparing these two figures clearly shows that the hexagonal base multi-domain lens 784 of the present invention exhibits at least the same performance as the spherical lens 792. The central area 789 of the hexagonal base multi-area lens 784 provides high image resolution and shallow depth of field at a wide range of views.

Each of the six side regions 796 of the hexagonal base multi-region lens 784 of the present invention has a focal length that depends on the position of the region in a complex manner, but the effect is as shown in FIG. 32. To spread over a range of values 798 corresponding to approximately +/- 10 percent of the center area focus. This vertical blurring of focus 798 effectively increases the depth of field of the lens in these areas 796 and provides the same benefits as having a flat-field lens. The performance of the outer region 800 of the spherical lens 792 can be seen in FIG. The vertical blurring of the focus 802 is significantly less in the spherical lens 792 than in the hexagonal base multi-domain lens 784.

This is particularly important for abnormal observations: increased depth of field and virtually outstanding depth of field alleviate the sudden image defocus that may occur in spherical lenses when the curved focal plane of the spherical lens is separated from the icon plane. Thus, unison material using a hexagonal base multi-domain lens displays a composite image that is softer away from focus at higher viewing angles than comparable unison material using spherical lenses. This is desirable because it increases the effective viewing angle of the material and thus increases its use as a security device or image rendering device.

The corner area 806 of the hexagonal base multi-area lens 784 of FIG. 32 provides the surprising advantage of scattering 808 the ambient light onto the icon plane and thus reduces the sensitivity of the unison material to the lighting condition. Has divergent focus characteristics. The spherical lens 792 of FIG. 33 does not scatter ambient light over a large area (visible by the absence of light rays scattered into the icon plane region 804), so that unison material made using the spherical lens may be viewed at various angles. In view of the above, the variation of the synthesized image brightness is larger than that of the unison material manufactured using the hexagonal base multi-domain lens.

The advantages obtained from the exemplary hexagonal base multi-domain lens are further magnified because the hexagonal base multi-domain lens has a higher filling rate (plane cover capability) compared to the spherical lens. The intergrid space between the spherical lenses virtually scatters no ambient light, and this non-scattering area is smaller in the case of hexagonal base multi-domain lenses.

Thus, although the focusing characteristics of the hexagonal base multi-domain lens are less than that of the spherical lens when evaluated by the conventional optical standard, in the context of the present invention, the hexagonal base multi-region lens provides unexpected advantages and advantages over the spherical lens. do.

Any type of lens may benefit from the addition of scattering microstructures or scattering materials that are incorporated or incorporated into the inter-lens grating space to enhance ambient illumination scattering onto the icon plane. In addition, the space between the lens gratings may be filled with a material forming a small diameter meniscus having converging or divergent focal characteristics to direct ambient illumination onto the icon plane. These methods can be combined, for example, by including light scattering particles in the lens lattice meniscus filling material. Alternatively, the inter lens lattice region may initially be made of a moderately scattering inter lens lattice region.

Spherical lenses having these properties are very difficult to manufacture because the large contact angle between the film surface and the lens edge acts as a stress concentrator for the force applied to separate the lens from the tool during manufacture. This high stress results in failure of lens adhesion to the film and failure of lens removal from the tool. Also, the optical performance of the low F # spherical lens is gradually degraded in the radial region far from the center of the lens, and the low F # spherical lens is poorly focused except near its center region.

Hexagonal base lenses have a surprisingly significant advantage over lenses with more nearly circular bases, and hexagonal lenses are released from the tool with a lower peel force than optically equivalent lenses with nearly circular bases. Hexagonal lenses are shapes that are mixed from nearly axially symmetrical to hexagonally symmetrical about their center and have a shape with corners that act as stress concentrators at their bases. The stress concentration caused by the sharp base corners reduces the total peel force required to separate the lens from its mold during manufacture. The degree of this effect is significant: the peel force can be reduced during manufacture by more than one factor for the hexagonal base lens compared to the nearly circular base lens.

Image contrast of the material can be enhanced by filling the inter-lens grating space with a light absorbing (black) opaque coloring material forming a mask for the lens. This eliminates the contrast reduction due to light scattered from the icon layer through the inter-lens grid. An additional effect of this intergrid filling is that the entire image is darker because the incoming ambient light cannot be introduced into the icon plane through the intergrid space. Image transparency produced by a lens having an aberrant focusing around it can also be improved by opaque colored intergrid filling, which occludes the abnormal peripheral lens area.

Other effects can be obtained by filling the inter-lens grating space with a white or light colored material, or with a material of a color that matches the substrate to be used with the unison material. If the filling between the light-colored lens grids is sufficiently dense and the icon plane has a strong contrast between the icon element and the background, the unison composite image will hardly be seen in reflected light, and clearly visible in transmitted light on the lens side. You will see it, but not from the icon side. This provides a novel security effect with a unidirectionally transmitted image that can only be seen with transmitted light and can only be seen on one side.

In the inter-lens lattice coating, fluorescent materials may be used in place of or in addition to the visible pigments to provide additional means of authentication.

4 illustrates the effect of changing the stereoscopic scale ratio (SSR) (icon element repetition period / lens array repetition period) along the axis of the material of the present invention. Areas of the system with SSRs greater than 1.000 will produce Unison float and superfloat effects, and areas with SSRs of nearly 1.000 will generate Unison motion parallax motion (OPM) effects, with SSRs less than 1.0000. The zone will generate the Unison Dip and Unison Superdeep effects. All of these effects can be created and transferred one by one in various ways along the axis of the system film. This figure shows one of infinitely various such combinations. The dotted line 66 indicates an SSR value almost corresponding to 1.000, which is a dividing line between the unison dip and unison superdip and unison float and unison superfloat, and an SSR value indicating OPM. In region 68 the SSR of the unison material is 0.005, producing a unison dip effect.

In the neighboring region 70, the SSR inclines from 0.995 to 1.005, creating a spatial transition from the unison dip to the unison float effect. In the next area 72, the SSR is 1.005, which produces the unison float effect. The next area 74 creates a smooth downward transition from the unison float effect to the unison dip effect. Area 76 moves forward cascading from the unison dip effect to the OPM, unison float effect, and area 78 goes back to the OPM. Changing the repetition period required to achieve these effects is generally easiest to perform in the icon element layer. In addition to changing the SSR in each area, it is desirable to change the rotation angle of each area of the array within the icon element array in order to keep the composite enlarged image at about the same size.

The easiest way to interpret this graph is to look at the graph as a cross-sectional view of the stereoscopic depth that will be perceived across this axis of one system material. Thus, it is possible to generate a sculpted field, shaping visual plane of the image by local control of the SSR and optionally by corresponding local control of the array rotation angle. This sterilized surface can be used to represent an unlimited range of shapes, including human faces. Patterns of icon elements that produce the effect of steric eroded grids or periodic dots can be a particularly effective way to visually display complex surfaces.

5A-C are plan views showing the effect of rotating one array pattern against another in fabricating the system of the present invention. 5A shows a lens array 80 having a regular periodic array spacing 82 with little change in angle of the array axis. 5B shows an icon element array 84 in which the array axis orientation angle 86 gradually changes. When lens array 80 is combined with icon element array 84 by moving the lens array over the icon array, the resulting approximate visual effect is shown in FIG. 5C. In FIG. 5C, the material 88 produced by the combination of the lens array 80 and the icon array 84 is a pattern of composite enlarged images 89, 90, 91 whose scale and rotation vary across the material. Create The image 89 facing the lower left end of the material 88 is large and shows no rotation at all. The image 90 facing the upper middle section of the material 88 is smaller and rotates a significant angle with respect to the image 89. The different scales and rotations between the images 89, 90 are the result of the difference in the angular misalignment of the lens pattern 82 and the icon element pattern 86.

6A-C illustrate a method for morphing one composite enlarged OPM image 98 into another composite enlarged image 102 as the first image moves across the boundary of the icon element pattern 92, 94. FIG. Illustrated. Icon element pattern 92 includes a circular icon element 98 shown in enlarged insert 96. Icon element pattern 94 includes star icon element 102 shown in enlarged insert 100. Icon element patterns 92 and 94 are not separate objects and are connected at their boundaries 104. When the material is assembled using this combined icon element pattern, the resulting OPM image exhibits the morphing effect shown in Figures 6B and C. 6B shows an OPM circular image 98 that appears as a star image 102 that moves across the boundary 104 to the right 107 and also moves to the right at the boundary. Image 106 has a partial circular and partial star shape when crossing boundaries during transition. 6C in the figure shows the image after further moving to the right, where image 98 is now closer to the border 104 and image 106 is nearly bordered to complete the morph from circular to star shape. Passing by. The morphing effect can be achieved in a less radical manner by creating transition regions from one icon element pattern to another instead of having a firm border 104. In the transition zone, the icon will change gradually from circle to star through a series of steps. The smoothness of the visual morphing of the resulting OPM picture will depend on the number of steps used for the transition. The range of graphical possibilities is infinite. For example, the transition region may be designed to shrink the circle while the sharp star point protrudes, or alternatively the side of the circle creates a blunt star that is progressively sharper until it reaches its final design. May be concave inwardly.

7A-C are cross-sectional views of the material of the system of the present invention, showing another embodiment of an icon element. FIG. 7A shows the material with the lens 1 separated from the icon element 108 by the optical spacer 5. The icon element 108 is formed by a pattern of colorless, colored, colored, or dyed material applied to the bottom surface of the optical spacer 5. In order to accumulate this kind of icon element 108 as long as the print resolution is accurate enough, many conventional methods such as inkjet, laserjet, letterpress, flexo, gravure, and intaglio can be used. Any of the in print methods can be used.

7B shows a similar material system with another embodiment of icon element 112. In this embodiment, the icon element is formed of pigments, dyes, or particles embedded in the substrate 110. Examples of the icon element 112 of this embodiment in the substrate 110 include silver particles in gelatin as a photo emulsion, pigment or dye ink absorbed in the ink receptor coating, dye sublimation transfer into the dye receptor coating, and in the imaging film. Photochromic or thermochromic images are included.

7C shows a microstructure method for forming the icon element 11. This method has the advantage of an almost unlimited spatial resolution. Icon element 114 may be formed alone or in combination from voids in microstructure 113 or solid region 115. These voids 113 may optionally be filled or coated with other materials, such as evaporated metal materials or dyeing or coloring materials having different refractive indices.

8A-B show a positive and negative embodiment of the icon element. 8A shows the positive icon element 116 colored, dyed or colored against a transparent background 118. 8B shows a negative icon element 122 transparent to a colored, dyed or colored background 120. The material of the system may optionally include positive and negative icon elements. This method of generating positive and negative icon elements is particularly suitable for the microstructure icon element of FIG. 7C.

9 is a cross-sectional view of one embodiment of a pixel-region material of the present system. This embodiment has an area with short focus lens 124 and another area with long focus lens 136. The short focus lens 124 projects an image 123 of the icon element 129 onto the icon plane 128 disposed in the focal plane of the lens 124. Long focal lens 136 projects an image 134 of icon element 137 onto icon plane 132 disposed in the focal plane of lens 136. Optical separator 126 separates short focus lens 124 from its associated icon plane 128. The long focal lens 136 is separated from its associated icon plane 132 by the sum of the thicknesses of the optical separator 126, the icon plane 128, and the second optical separator 130. The icon element 137 on the second icon plane 132 is located outside the depth of focus of the short focus lens 124 and thus does not form a separate composite enlarged image in the short focus lens region. Similarly, icon element 129 is too close to long focal lens 136 to form a separate composite enlarged image. Thus, the material region supporting the short focus lens 124 will display an image 123 of the icon element 129, and the material region supporting the long focus lens 136 will display an image 134 of the icon element 137. Will be displayed. Projected images 123 and 134 may differ in effects including the design, color, OPM direction, composite magnification factor, and dip, union, float, and flotation effects described above.

10 is a cross-sectional view of another embodiment of a pixel-region material of the present system. This embodiment has an area with the lens 140 raised by a lens support mesa 144 on the base of the non-elevated lens 148. The focal length of the raised lens 140 is a distance 158, which places the focal points of these lenses on the first icon plane 152. The focal length of the non-elevated lenses 148 is a distance of 160, placing the focal points of these lenses on the second icon plane 156. These two focal lengths 158, 160 project an image 138 of the icon element 162 onto the icon plane 152 disposed in the focal plane of the lens 140. Elevated lens 148 projects image 146 of icon element 164 onto icon plane 156 disposed in the focal plane of lens 148. The raised lens 140 is separated from its associated icon element 162 by the sum of the thicknesses of the lens support mesa 144 and the optical separator 150. Elevated lens 148 is separated from its associated icon element 164 by the sum of the thicknesses of optical separator 150, icon layer 152, and icon separator 154. The icon element 164 in the second icon plane 156 is located outside the depth of focus of the raised lens 140 and thus does not form a separate composite enlarged image in the raised lens area. Similarly, icon element 152 is too close to the non-elevated lens 148 to form a separate composite enlarged image. Thus, the material region supporting the raised lens 140 will display an image 138 of the icon element 162, and the material region supporting the non-elevated lens 136 will display an image of the icon element 156. 146). The projected images 138, 146 may differ in design, color, OPM direction, composite magnification factor, and effects including dip, union, float, and flotation effects.

11A and 11B are cross-sectional views showing a non-refractive embodiment of the present system. 11A illustrates an embodiment of using focusing reflector 166 instead of a refractive lens to project an image 174 of icon element 172. Icon layer 170 lies between the observer's eye and the focusing optics. Focusing reflector 166 may be metallized 167 to achieve high focusing efficiency. The icon layer 170 is maintained at the same distance as the focal length of the reflector by the optical separator 168. 11B shows a pinhole optical embodiment of this material. An opening 178 is formed through the transparent upper layer 176 where black for contrast enhancement is desired. Optical separator element 180 controls the field of view of the system. Icon element 184 of icon layer 182 is imaged through opening 178 in a manner similar to the pinhole optics of a pinhole camera. Since the amount of light passing through the opening is small, this embodiment is most effective when it is back illuminated by light passing first through the icon plane 182 and then through the opening 178. The effects of each of the above embodiments, namely OPM, dip, float, and flotation effects, can be generated using either a reflection system design or a pinhole optical system design.

12A-B are cross-sectional views comparing the structure of an all-refractive material 188 with the structure of a hybrid refracted / reflective material 199. 12A shows an exemplary structure in which micro-lens 192 is separated from icon plane 194 by optical separator 198. The optional sealing layer 195 contributes to the pre-refractive system thickness 196. Lens 192 projects icon image 190 towards an observer (not shown). Hybrid refractive / reflective material 199 includes a micro-lens 210 with an icon plane 208 directly below it. Optical spacer 200 separates lens 210 and icon plane 208 from reflective layer 202. Reflective layer 202 may be metallized, for example, by evaporated or sputtered aluminum, gold, rhodium, chromium, osmium, depleted uranium or silver, by chemically deposited silver, or by a multilayer interference film. have. Light scattered from the icon layer 208 is reflected from the reflective layer 202 and travels through the icon layer 208 into the lens 210, which projects the image 206 towards the viewer (not shown). . Both of these figures are drawn on approximately the same scale, and visual comparison shows that the overall system thickness 212 of the hybrid refraction / reflection system 199 is approximately half of the overall system thickness 196 of the pre-refraction system 188. It can be seen that. Exemplary dimensions of equivalent systems are 29 μ for prerefractive system 188 thickness 196 and 17 μ for total hybrid refraction / reflection system 199 thickness 212. The thickness of the refraction / reflection system can be further reduced by scaling. Thus, hybrid systems with lenses of 15μ diameter can be manufactured to an overall thickness of approximately 8μ. The effects, OPM, dip, float, flotation, morph, and 3-D effects of each of the above embodiments can be generated using a hybrid refraction / reflection design.

Figure 13 is a cross-sectional view illustrating an embodiment of a 'peel-to-reveal' tamper-indicating material of the present system. This embodiment does not display an image until it is unsealed. An untampered structure is shown in region 224, where the refractive system 214 consists of a peelable layer 220 matching the optional substrate 218 and the lens 215. It is optically embedded under the upper layer 216. The peelable layer 220 effectively forms a negative lens structure 220 that fits over the positive lens 215 and negates its optical power. Lens 215 cannot form an image of the icon layer in an unopened region, and light scattered 222 from the icon plane is not focused. Upper layer 216 may have an optional film substrate 218. Unsealed, shown in area 226, causes release of upper layer 216 from refractive system 214 and exposes lens 215 to form image 228. The effects, OPM, dip, float, and flotation of each of the above embodiments can be included in the tamper resistant 'peel-exposure' system of the type of FIG.

Fig. 14 is a sectional view showing an embodiment of a 'peel-change' tamper resistant material of the present system. This embodiment displays the first image 248 of the first icon plane 242 before the tamper 252 and the second image 258 in the region 254 after tampering. The unopened structure is shown in area 252 where two refracting systems 232, 230 are stacked. The first icon plane 242 is located under the lens 240 of the second system. Prior to tampering in area 252, first or upper system 232 presents an image of first icon plane 242. The second icon plane 246 is too far outside of the depth of focus of the lens 234 to form a separate image. The first lens 234 is separated from the second lens 240 by a peelable layer 238 that conforms to the optional substrate 236 and the second lens 240. The peelable layer 232 effectively forms a negative lens structure 238 that fits over the positive lens 240 and negates its optical power. Upper layer 232 may include an optional film substrate 236. Misopening shown in region 254 causes release of upper layer 232 from second refraction system 230 and causes second lens 240 to form an image 258 of second icon layer 246. Expose The second lens 240 does not form an image of the first icon layer because the first icon layer 242 is too close to the lens 240.

This embodiment of tamper resistant material is suitable for application as tape or label applied to articles. The tamper release releases the top layer 232 and attaches the second system 230 to the article. Prior to tampering, this embodiment produces a first image 248. After the tamper 254, the second system 230 still attached to the article shows a second image 258, and the peelable layer 256 shows no image. The effects, OPM, dip, float, and flotation of each of the above embodiments may be included in the first system 232 or the second system 230.

It should be noted that a variant that achieves an effect similar to that of Figure 14 includes two separate systems that are stacked together. In this modification, the first icon plane and its image are removed when the upper layer is peeled off, and the second system and its image are exposed.

15A-D are cross sectional views showing a two-sided embodiment of the present system. 15A illustrates a double-sided material having a single icon plane 264 in which an image 268 is formed by a lens 262 on one side and an image 270 by a second set of lenses 266 on the opposite side. 260 is shown. The image 268 viewed from the left side of the figure is a mirror image of the image 270 viewed from the right side. Icon plane 264 may include an icon element that is a symbol or image that looks similar in a mirror image, or an icon element that looks different in a mirror image, or a combination of icon elements, where some of the icon elements are viewed from one side. It is read correctly and the other icon elements are read correctly when viewed from the other side. The effects, OPM, dip, float, and flotation of each of the above embodiments can be displayed on both sides of the double-sided material according to this embodiment.

FIG. 15B shows another double sided embodiment 272 having two icon planes 276, 278 formed by two sets of lenses 274, 280, respectively, images 282, 286. This embodiment is essentially two separate systems 287 and 289 as shown in FIG. 1A connected with an icon layer spacer 277 therebetween. The thickness of this icon layer spacer 277 will determine the extent to which the 'wrong' icon layer is formed by images 284 and 288 by the lens set. For example, if the thickness of the icon layer spacer 277 is zero such that the icon layers 276 and 278 contact, both icon layers will be imaged by both sets of lenses 274 and 280. In another example, if the thickness of the icon layer spacer 277 is significantly greater than the depth of focus of the lenses 274, 280, the 'wrong' icon layer will not be imaged by the lenses 274, 280. In another example, if the depth of focus of one set of lenses 274 is large but the depth of focus of another set of lenses is small (because the lenses 274, 280 have different F # s), then both icon planes 276, 278 ) Will be imaged 282 through lens 274, but only one icon plane 278 will be imaged through lens 280, so this type of material will show two images from one side. One of these images is a mirror image from the opposite side. Each effect, OPM, dip, float, and flotation of the above embodiments may be displayed on both sides of the double-sided material according to the present embodiment, and the projected images 282 and 286 may be the same or different colors.

15C shows another double sided material 290 having a colored icon layer spacer 298 that prevents the lens on one side of the material from seeing the 'wrong' icon set. Lens 292 forms image 294 on icon layer 296 due to the presence of colored icon layer 298 but cannot form image on icon layer 300. Likewise, lens 302 forms an image 304 on icon layer 300 due to the presence of colored icon layer 298 but cannot form an image on icon layer 296. The effects, OPM, dip, float, and flotation of each of the above embodiments can be displayed on both sides of the double-sided material according to this embodiment, and the projected images 294 and 304 can be the same or different colors.

FIG. 15D illustrates an additional double sided material 306 embodiment having a lens 308 that forms an image 318 in an icon layer 314, and a lens 316 that forms an image 322 in an icon layer 310. Illustrated. Icon layer 310 is in close or near contact with the base of lens 308, and icon layer 314 is in close or near contact with base of lens 316. Icon 310 is too close to lens 308 to form an image, so that light is scattered 320 instead of focusing. Icon 314 is too close to lens 316 to form an image, so that light is scattered 324 instead of focusing. The effects, OPM, dip, float, and flotation of each of the above embodiments can be displayed on both sides of the double-sided material according to the present embodiment, and the projected images 318 and 322 can be the same or different colors.

16A-F are cross sectional and corresponding top views illustrating three different methods for generating a grayscale or tonal icon element pattern with the system of the present invention and subsequently creating a composite enlarged image. 16A-C are detailed cross-sectional views of an icon side of material 307 having a portion of optical separator 309 and a transparent microstructure icon layer 311. The icon element is formed as a bas-relief surface 313, 315, 317 filled with colored or dyed material 323, 325, 327, respectively. The bottom surface of the icon layer may optionally be sealed by a sealing layer 321 that may be transparent, colored, colored, dyed, or colored or opaque. The shallow relief microstructure of the icon elements 313, 315, and 317 provides a change in thickness to each of the dyed or colored fill materials 323, 325, and 327, which, as shown in the plan view, changes the optical density of the icon element. Create Top views corresponding to icon elements 323, 325, and 327 are top views 337, 339, and 341. The use of this method for generating a gradation or tonal synthesis magnified image is not limited to the specific examples disclosed herein, and may generally be applied to generate various gradation images indefinitely.

16A shows icon element 313, dyed or colored icon element fill 323, and corresponding plan view 337. A cross-sectional view of the icon plane above this figure may only show one cutting plane through the icon element. The location of the cutting plane is shown by the dotted line 319 through the top views 337, 339, 341. Thus, the cross section of the icon element 313 is one plane passing through a nearly hemispherical icon element. By appropriately limiting the total dye or pigment concentration of the fill 323, the thickness change of the dyed or colored fill 323 creates a hue, or gradation, optical density change that appears in plan 337. An array of icon elements of this type can be composited and enlarged within the present material system to produce an image representing an equivalent gradation change.

16B shows icon element 315, dyed or colored icon element fill 325, and corresponding plan view 339. Floor plan 339 shows that icon element 315 depicts a shallow relief of the face. The color tone change in the face image is complex, as shown by the complex thickness change 325 in the cross-sectional view. As shown for icon element 313, an array of icon elements of this type, shown as 315, 325, and 339, is synthesized within the present material system to produce an image representing an equivalent gradation change representing a face image in this example. Can be enlarged.

16C shows icon element 317, dyed or colored fill 327, and corresponding plan view 341. As discussed in Figures 16A and B above, the shallow relief shape of this icon element structure produces a hue change in the appearance of the dyed and colored fill 327, and the composite enlarged image produced by the present material system. do. Icon element 317 illustrates a method for creating a bright center on a rounded surface compared to the effect of icon element 313 on creating a dark center on a rounded surface.

16D, E illustrate another embodiment 326 of a transparent shallow relief microstructured icon layer 311 with icon elements 329 and 331 coated with a high refractive index material 328. FIG. The icon layer 311 may be sealed with an optional sealing layer 321 that fills the icon elements 329, 331; 330, 332, respectively. The high refractive index layer 328 improves the visibility of the inclined surface by generating reflections from the inclined surface by total internal reflection. The top views 342 and 344 represent representative images of the appearance of the icon elements 329 and 331, and composite enlarged images thereof. This high refractive index coating embodiment provides a kind of edge-enhancing effect without adding pigments or dyes to make the icon and its image visible.

16F illustrates another embodiment 333 of a transparent shallow relief microstructure icon 335 that uses air, gas, or liquid volume 336 to visually define this phase interface 334 microstructure. ). An optional sealing layer 340 can be added with or without the optional adhesive 338 to capture the air, gas, or liquid volume 336. The visual effect of the phase interface icon element is similar to the visual effect of the high refractive index coated icon element 329, 331.

17A-D are cross sectional views illustrating the use of the present system as a laminated film with printed information such as may be used to manufacture ID cards and driver's licenses, where (as described above with a systematic micro-array of lenses and images). Material 348) covers a substantial portion of the surface. FIG. 17A shows an embodiment of Unison used as a laminate on a print 347. A material 348 having at least some optical transparency in the icon layer is laminated to a fibrous substrate 354, such as paper or a paper substitute, by a laminating adhesive 350, which adhesive is previously applied to the fibrous substrate 354. Cover or partially cover print element 352. Because the material 348 is at least partially transparent, the print element 352 can be seen through it, and the effect of this combination is to provide the dynamic image effect of the present system in combination with the static print.

FIG. 17B shows an embodiment of a system material used as a laminate over a print element 352 applied to a non-fibrous substrate 358 such as a polymer film. As shown in Fig. 17A, a material 348 having at least some optical transparency in the icon layer is laminated to a non-fibrous substrate 358, such as a polymer, metal, glass, or ceramic substitute, by a laminating adhesive 350, The adhesive covers or partially covers the print element 352 previously applied to the non-fibrous substrate 354. Because the material 348 is at least partially transparent, the print element 352 can be seen through it, and the effect of this combination is to provide a dynamic picture effect in combination with a static print.

17C illustrates the use of a print element directly on the lens side of material 360. In this embodiment material 348 has a print element 352 applied directly to the image lens surface. This embodiment does not require the material to be at least partially transparent: the print element 352 is placed on top of the material and a dynamic picture effect can be seen around the print element. In this embodiment, material 348 is used as a substrate for finished products, such as bills, ID cards, and other articles that require authentication or provide authentication to other articles.

17D illustrates the use of a print element directly on the icon side of at least partially transparent material 362. Print element 352 is applied directly to an icon layer or sealing layer of at least partially transparent system material 348. Since the system material 348 is at least partially transparent, the print element 352 can be seen through it, and the effect of this combination is to provide a dynamic picture effect in combination with a static print. In this embodiment system material 348 is used as a substrate for finished products, such as bills, ID cards, and other articles that require authentication or provide authentication to other articles.

Each of the embodiments of Figs. 17A-D may be used alone or in combination. Thus, for example, system material 348 may be overprinted (FIG. 17C) and backside printed (FIG. 17D) and then optionally laminated (FIGS. 17A, B) onto a print on a substrate. Combinations such as these can further increase the forgery, imitation, and tamper resistance of the materials of the present system.

18A-F illustrate the application or incorporation of the present system to various substrates in combination with printed information. While FIGS. 17A-D disclose a system material 348 that covers most or all of an article, FIGS. 18A-F show that the system material or its optical effect does not substantially cover the entire surface but rather only a portion of the surface. The embodiment of Figs. 18A-F is different from the embodiment of Figs. 17A-D in that it discloses an embodiment. 18A shows a portion of at least partially transparent system material 364 adhered to a fibrous or non-fibrous substrate 368 by an adhesive element 366. An optional print element 370 was applied directly to the upper lens surface of the material 364. The print element 370 may be part of a large pattern extending beyond a portion of the material 364. A portion of the material 364 is optionally laminated over the print element 372 applied to the fibrous or non-fibrous substrate prior to the application of the material 364.

18B shows an example of a cross-sectional system material 364 incorporated as a window to a non-optical substrate 378, where at least a portion of the edge of the system material 364 is captured by the non-optical substrate 378, Cover, or be surrounded. The print element 380 may be selectively applied on top of the system material lens surface, and these print elements may be aligned with the print element 382 applied to the non-optical substrate 378 in the region adjacent the print element 380 or Can match that. Similarly, print element 384 may be applied to the opposite side of the non-optical substrate that is aligned or coincident with the icon of system material 364 or print element 386 applied to sealing layer 388. The effect of this kind of window is to provide a one-sided image effect by displaying the individual images when the material is viewed from the lens side and no images when viewed from the icon side.

FIG. 18C illustrates an embodiment similar to FIG. 18B except that system material 306 is double-sided material 306 (or the double-sided embodiment described above). The print elements 390, 392, 394, 396 are almost identical in function to the print elements 380, 382, 384, 386 described above. The effect of this kind of material window would result in different individual images when looking at the material from both sides. For example, a window included in a bill paper may display a number sign of a bill such as "10" when viewed from the front of the bill, but when viewed from the back of the bill, the Unison window may be the same color as the first image or Other information may be displayed, such as "USA", which may be of a different color.

18D shows a transparent substrate 373 acting as an optical spacer for the material formed by the limited degree of lens 374 region, and an icon layer 376 extending significantly beyond the perimeter of the lens 374 region. . In this embodiment, the effect of the present invention will be seen only in the area having both the lens and the icon (in this figure corresponds to the lens area 374). Both the lens 374 and the adjacent substrate may be selectively printed 375, the print element also having an icon layer 376 or an optional sealing layer covering the icon (not shown in this figure, see FIG. 1). It can be applied to. After the manner of the present embodiment, the article may use a plurality of lens regions, and wherever the lens regions are located, the unison effect will be seen. The size, rotation, stereoscopic depth position, and OPM characteristics of the image may be The lens area may vary. This embodiment is suitable for application to ID cards, credit cards, driver's licenses, and similar applications.

18E illustrates an embodiment similar to FIG. 18D except that icon plane 402 does not substantially extend beyond the size of lens area 400. Optical spacer 398 separates lens 400 from icon 402. Print elements 404 and 406 correspond to print elements 375 and 377 in FIG. 18D. After the manner of this embodiment, multiple regions 400 may be used in the article, each of which may have a separate effect. This embodiment is suitable for application to ID cards, credit cards, driver's licenses, and similar applications.

FIG. 18F illustrates an embodiment similar to FIG. 18D except that the present embodiment includes an optical spacer 408 that separates lens 413 from icon plane 410. Lens 413 extends significantly beyond the perimeter of icon area 412. Print elements 414 and 416 correspond to print elements 375 and 377 in FIG. 18D. After the manner of this embodiment, a plurality of lens areas may be used in the article, where the effect will be seen wherever the lens areas are placed; The size, rotation, stereoscopic depth position, and OPM characteristics of the image may be different for each lens region. This embodiment is suitable for application to ID cards, credit cards, driver's licenses, and similar applications.

19A-B show cross-sectional views that compare the in-focus field of view of a spherical lens with that of a plainfield aspheric lens, each of which is incorporated in a structure of the type described above. Fig. 19A shows a practical spherical lens when applied to the system described above. The substantially spherical lens 418 is separated from the icon plane 422 by the optical spacer 420. The image 424 projected perpendicular to the surface of the material originates in the focal point 426 in the icon layer 422. The image 424 is precisely focused because the focus 426 is located within the icon layer 422. Looking at the lens from an oblique angle, the image 428 is blurry and out of focus because the corresponding focus 430 does not lie in the icon plane and rises significantly above it. Arrow 432 represents the curvature of the lens corresponding to focal curvature from 426 to 430. The focus is in the icon plane in area 434 and moves out of the icon plane in area 436. Lenses suitable for applications that cooperate with the plane of the printed image or icon typically have a low F # of less than 1, resulting in very shallow focal depth-high F # lenses that can be effectively used with dip and float effects, When used together, it results in a proportional vertical binocular parallax with the effects described herein. As soon as the lower limit of the depth of focus moves out of the icon plane, the image sharpness drops sharply. As can be seen from this figure, the field of view curvature of the actual spherical lens limits the field of view of the image, and the image is clear only when in the focusing area 434 and rapidly defocused at a more inclined perspective. The actual spherical lens is not a plain field lens and its field of view curvature is magnified for low F # lenses.

Fig. 19B shows an aspherical lens applied to the present system. As an aspherical lens, its curvature is not close to the sphere. Aspheric lens 438 is separated from icon layer 442 by optical spacer 440. Aspheric lens 438 projects image 444 of icon plane 442 perpendicular to the plane of material. The image originates at the focus 446. The focal length of the aspherical lens 438 lies within the icon plane 442 for a wide range of views, from vertical 444 to inclined 448 because it has a plain field 452. The focal length of the lens depends on the view through it. The focal length is the shortest upon vertical observation 444 and increases as the vision gradually slopes. The focal point 450 is still within the thickness of the icon plane at the oblique time 448, so that the oblique image is still in focus at this oblique time 448. The focusing area 454 in the aspheric lens 438 is much wider than the focusing area 434 of the substantially spherical lens 418. Aspheric lens 438 thus provides an enlarged field of view relative to the width of the associated image icon, so that the peripheral edge of the associated image icon does not deviate from that of the spherical lens 418. Aspherical lenses are preferred for the present system because they provide a wider field of view and increase the visibility of the associated image.

20A-C are cross-sectional views illustrating two advantages in use resulting from the use of a thick icon layer. These benefits apply whether the lens 456 used for viewing is substantially spherical 418 or aspherical 438, but is greatest when combined with aspherical lens 438. 20A shows a thin icon layer 460 system material with a lens 456 separated from the icon layer 460 by an optical spacer 458. The icon element 462 is thinner than the curvature of the lens 463 (461) and limits the focusing area to a small angle, which is in the image and icon layer 460 projected in the vertical direction 464. The angle between the highest tilt angle image 468 with the focus 470. The maximum field of view is obtained by maximizing the tilt angle of view by designing the vertical image focus 466 at the bottom of the icon plane, limited by the point where the focus 470 lies at the top of the icon plane. The field of view of the system in FIG. 20A is limited to 30 degrees.

20B illustrates the benefits obtained by having a thick 472 icon plane 471 relative to the field of view curvature of the lens 456. Lens 456 is separated from thick icon element 474 by optical spacer 458. The thick icon element 474 remains focused 475 over a large 55 degree field of view compared to the thin icon element 462 of FIG. 20A. The vertical image 476 projected from the focus 478 through the lens 456 is in sharp focus, the focus being 55 where the tilted image 480 focus 482 lies on top of the thick icon plane 471. Maintain clarity while increasing vision up to degrees. The increased field of view is greatest in plain view lenses, such as the aspherical lens 438 of FIG. 19B.

20C illustrates another advantage of thick icon plane 492, which lowers the sensitivity of the present system material to changes in thickness S that may result from fabrication changes. The lens 484 is spaced apart by a distance S from the bottom surface of the icon layer of thickness i. Lens 484 projects the image 496 from the focus 498 disposed at the bottom of the icon layer 492. This figure is made to show that the variation of the optical distance S between the lens and the icon layer can vary over a range equivalent to the thickness of the icon layer i without losing the focus of the images 496, 500, 504. . The optical spacer thickness in the lens 486 is approximately (S + i / 2) and the focus 502 of the image 500 is still within the thickness i of the icon layer 492. The thickness of the optical spacer in lens 488 increases to (S + i) 490, and focus 506 of image 504 lies on top of thick icon element 494. Thus, the optical spacer thickness can vary over a range corresponding to the thickness of the icon layer (i), so that the thin icon layer provides a small tolerance for changes in the optical spacer thickness, and the thick icon layer provides a change in the optical spacer thickness variation. Provide large tolerances.

Additional advantages are provided by the thick icon layer 492. An incomplete lens, such as a substantially spherical lens, may have a short focal length 493 from its center 496 toward its edge. This is one aspect of the general spherical aberration defect of a practical spherical lens. The thick icon layer provides icon elements that can be sharply focused over a range of focal lengths 498 to 495, thus enhancing the overall sharpness and contrast of the image produced by the lens 484 with varying focal lengths. Let's do it.

Fig. 21 is a plan view showing that the system is applied as a 'windowed' security thread to banknotes and other security documents. Figure 21 illustrates a partially exposed hidden line structure with system material 508 slitted on a ribbon, referred to as a "silver line", typically in the range of 0.5mm to 10mm in width. Hidden lines 508 are included in the fibrous document substrate 510 and provide a partially exposed area 514. Hidden lines 508 may increase image contrast and / or provide additional security and authentication features such as electrical conductivity, magnetic properties, nuclear magnetic resonance detection and authentication, or may provide material back to the substrate (union composite image). Dyed, colored, filled, or coated sealing layer 516 to conceal from observation in reflected illumination when viewed from the opposite side) and to enhance the bond between the hidden line 508 and the fibrous substrate 510. An adhesive layer 517 may optionally be included. Hidden line 508 is maintained in an orientation that keeps the lens at the top so that image effects can be seen in partially exposed area 514. The fibrous substrate 510 and the silver wire may be overprinted by the print element 518 and the fibrous substrate may be printed 520 on the opposite side.

21 shows that the hidden line 508 and its image effect 522 can only be seen from the top surface 521 of the substrate 510 in the partially exposed area. Hidden line 508 is covered by the fibrous substrate in the inner region 512, where the image effect 522 is virtually invisible. The OPM effect is particularly dramatic when included in hidden line 508 (see Figure 22). When the fibrous substrate 510 is inclined in various directions, the OPM image can be made to scan across the width 524 of the hidden line to create a phenomenal and dramatic visual effect. This scanning feature of the OPM image may represent an image 522 that is larger than the width of the hidden line 508. A user inspecting a document in which the partially exposed hidden line 508 is housed may tilt the document to scan the entire image across the hidden line to scroll like a marquee sign. The effects of the dip, float, and flotation embodiments can also be advantageously used in the partially exposed hidden line format.

Hidden line 508 may be at least partly included in the security paper during manufacture by techniques commonly used in the paper industry. For example, the hidden line 508 may be pressed into the wet paper while the fiber is in an intact and flexible state, as disclosed in US Pat. No. 4,534,398, which is incorporated herein.

The partially exposed hidden line of the system is particularly suitable for application to banknotes. Typical total thickness of the silver wire material is in the range of 22 microns to 34 microns, and the total thickness of the banknote paper may range up to 88 microns. By locally reducing the thickness of the paper by the thickness of the hidden line, the partially exposed hidden line of the system can be included in the bill paper without substantially changing the overall thickness of the paper.

In an exemplary embodiment, the hidden line 508 is

(a) one or more optical spacers,

(b) one or more optionally periodic planar arrays of micro-pictures or icons disposed within, on, or adjacent to the optical spacer, and

(c) one or more optionally periodic planar arrays of non-cylindrical microlenses disposed on or adjacent to the optical spacer or planar icon array.

In another embodiment, the micro-images constitute fill voids or recesses formed on the surface of one or more optical spacers, wherein the non-cylindrical micro-lenses are aspherical micro-lenses, each aspherical micro-lens being approximately 15 to It has a base diameter of approximately 35 microns. At least one colored seal or occlusion in a flat array of micro-images or icons to increase contrast and thereby increase the visual acuity of the icon and to conceal the presence of hidden lines 508 when at least partially embedded in a secure document. Layer 516 may be disposed.

In another embodiment of the invention, the hidden line 508,

(a) one or more optical spacers having opposing upper and lower flat surfaces,

(b) a periodic array of micro-images or icons comprising filling recesses formed in the lower flat surface of the optical spacer,

(c) a periodic array of non-cylindrical, plain-field, aspherical, or polygonal base multi-region micro-lenses disposed on an upper flat surface of the optical spacer, each having a base diameter of approximately 20 to approximately 30 microns, and

(d) a colored seal or occlusion layer 516 disposed on the icon array.

Optical spacers may be formed using one or more essentially colorless polymers including, but not limited to, polyesters, polypropylenes, polyethylenes, polyethylene terephthalates, polyvinylidene chlorides, and the like. In an exemplary embodiment, the optical spacer is formed using polyester or polyethylene terephthalate and has a thickness of approximately 8 to 25 microns.

Icons and micro-lens arrays can be formed using substantially transparent or clear radiation curable materials, including but not limited to acrylics, polyesters, epoxies, urethanes, and the like. The array is preferably formed using an acrylated urethane sold under the name U107 from Lord Chemicals.

Each of the icon recesses formed in the lower flat surface of the optical spacer is approximately 0.5 to 8 microns in depth and micro-lens or icon width is typically 30 microns. The recess may be filled with any suitable material, such as colored resin, ink, dye, metal, or magnetic material. In an exemplary embodiment, the recess is filled with a colored resin comprising a sub-micron pigment sold under the name Spectra Pac from Sun Chemical Corporation.

Colored seal or occlusion layer 516 employs one or more of a variety of opaque coatings or inks including, but not limited to, colored coatings including pigments such as titanium dioxide dispersed in a binder or carrier of a curable polymer material. Can be formed. The sealing or occluding layer 516 is formed using a radiation curable polymer and preferably has a thickness of approximately 0.5 to 3 microns.

The hidden line 508 described above,

(a) applying a substantially transparent or clear radiation curable resin to the top and bottom surfaces of the optical spacer,

(b) forming a micro-lens array on the upper surface of the optical spacer and a recessed icon array on the lower surface thereof;

(c) curing the substantially transparent or clear resin using a radiation source,

(d) filling the icon array recess with colored resin or ink,

(e) removing excess resin or ink from the bottom surface of the optical spacer, and

and (f) applying a colored sealing or occlusive coating layer to the lower surface of the optical spacer.

In many cases, secure hidden lines used in banknotes and other expensive financial and identification documents are detected and authenticated by high-speed non-contact sensors such as capacitive sensors, magnetic field sensors, optical transmission and opacity sensors, fluorescence, and / or nuclear magnetic resonance. It is preferable to be.

Inclusion of fluorescent material in the lens, substrate, icon matrix, or icon fill element of the Unison film allows the Unison material to be concealed or forensically certified by the observation of the presence of fluorescence and spectral characteristics. The fluorescent unison film can be designed so that its fluorescence properties can be seen on both sides of the material or only on one side. If there is no optical isolation layer in the material below the icon layer, the fluorescence of any portion of the unison material can be seen on both sides. The inclusion of an optical isolation layer allows separation of the visibility of fluorescence on both sides. Thus, Unison materials comprising an optical isolation layer below the icon plane can be designed to fluoresce in a number of different ways: fluorescent color A visible from the lens side, fluorescent light not visible from the optical isolation layer, optical isolation layer. Fluorescent color A or B visible from the side but not from the lens side, and fluorescent color A visible from the lens side, and fluorescent color A or B visible from the optical isolation layer side. Specificity that can be used can be used to further improve the security of the Unison material. The optical isolation layer can be a layer of colored or dyed material, a metal layer, or a combination of colored and metal layers that absorbs or reflects fluorescence emission from one side of the material and prevents it from being seen from the other side.

Molded voids and vice versa shaped icons, icons formed of molded posts, enable the addition of machine-readable authentication features, in particular to unisex material security hidden lines for banknotes and other expensive documents. Icon matrix, icon fill, and any number of back coats (sealing coats) include non-fluorescent pigments, non-fluorescent dyes, fluorescent pigments, fluorescent dyes, metal particles, magnetic particles, nuclear magnetic resonance signature materials, oscillation particles, organic LED materials, Optically variable materials, evaporated metals, thin film interface materials, liquid crystal polymers, optical upconversion and downconversion materials, dichroic materials, optically active materials (with optical rotational power), optical polarizing materials, and other associated materials, Individually and / or in any combination.

In some situations, such as when a black or color coating (such as a magnetic material or conductive layer) is added to a Unix material or when the color of the icon plane can be observed when viewed from the back of the substrate, buried, partially buried, or partially It may be desirable to conceal or shield the appearance of exposed Unix material security hidden lines from reflected light from one side of the paper substrate and to allow the hidden lines to be visible from opposite sides of the substrate. Other forms of banknote security hidden lines typically include a metal layer, typically an aluminum layer, to reflect light filtered through the surface substrate to provide similar brightness to the surrounding substrate. Likewise, aluminum or other color neutral reflective metal can be used to conceal the appearance of the unison hidden wire from the back of the paper substrate by applying a metal layer to the back of the unison material and optionally sealing it in place. A colored layer can be used instead of or with the metal layer for the same purpose, which blocks the visibility of the security hidden line at the back of the document. The colored layer may be any color, including white, but the most effective color is one that matches the color and intensity of light scattered inside or outside of the fibrous substrate.

The addition of the metallized layer to the unison material may include direct metallization of the icon or sealing layer of unison material by evaporation, sputtering, chemical vapor deposition, or other suitable means, or unison to the metallized surface of the second polymer film. It can be done in a variety of ways, including lamination of the icon or sealing layer of material. Metallization of the film, patterned metallization of the film, leaving a narrow 'ribbon' of the metallized area, laminating the metallized surface to the second polymer film, and then slitting the laminated material to form a metal ribbon. It is a common procedure to create a banknote secure hidden line by protecting the metal from chemical attack at the hidden line edge by allowing it to be isolated from the edge of the slit hidden line by the lamination adhesive. This method can also be applied in the case of the present invention: unison material can simply replace the second laminated film. Thus, the union material can be reinforced by adding a patterned or unpatterned metallization layer.

The composite image can be designed as a binary pattern with one color (or absence of color) forming an icon and another color (or absence of color) forming a background, in which case each icon area is full on. ) Or a full monotone image using an image 'pixel' in the full off state. By providing a change in the hue of the selected icon color, a more complex composite image can be generated. The composite image hue change can be generated by controlling the color intensity in each icon image, or by effectively 'half-toning' the composite image by including or excluding design elements in the selected icon group.

The first method of controlling the color density in each icon image can be achieved by controlling the optical density of the material producing the microprinted icon image. One convenient way to do this uses the fill void icon embodiment described above.

A second method of 'dotting' a composite image by including or excluding design elements in the selected icon group shown in FIG. 23 is achieved by providing image design elements at a ratio of an icon area equal to a predetermined color density. Figure 23 shows an example of using a hexagonal icon area 570 repeating pattern to cooperate with a similar hexagonal repeating lens pattern. Each of the icon areas 570 does not have the same information. The entirety of the icon image elements 572, 574, 576, and 578 are present at about the same color density. Icon picture elements 572 and 574 exist in some icon areas, while other icon picture elements exist in other icon areas. Some icon areas include a single icon picture element 570. Specifically, the icon picture element 572 is in half of the icon area, the icon picture element 574 is in three quarters of the icon area, the icon picture element 578 is in half of the icon area, The icon picture element 576 is present in 1/3 of the icon area. The information present in each image area determines whether the associated lens shows the color of the icon image pattern or the color of the icon image background from a particular viewing orientation. Any image element 572 or 578 can be seen in all lenses associated with this icon pattern, but the composite image 580 space of the icon image element 572 overlaps with the composite image space of the icon image element 578. This means that the overlap area 582 of the composite image of the icons 572 and 578 appears to be 100% color density because all the lenses project the icon image in this area. The non-overlapping portion 588 of these two composite images is only visible at 50% of the lens, and therefore is seen at 50% color depth. The composite image 586 of the icon element 576 can only be seen in one third of the lens, so it appears to be at 33.3% concentration. The composite image 584 of the icon image element 576 appears to be correspondingly at 75% color depth. It is evident within the scope of this teaching that a significant range of tonal changes can be obtained through selective omission of icon picture elements at a selected percentage of the icon area. For maximum effect, the distribution of icon picture elements across the icon picture area should be relatively uniform.

In order to produce a combined composite image element of dimensions smaller than the minimum features of the individual composite image elements, the associated icon image design method shown in Fig. 24A can be used. This is possible in general situations where the minimum feature size of the icon picture is greater than the placement accuracy of the feature. Thus, the icon image may have a minimum feature on the order of 2 microns in dimension, but these features may be accurately placed at any point on the grid at 0.25 micron intervals. In this case, the minimum feature of the icon image is eight times larger than the placement accuracy of the feature. As in the previous figure, this method is shown using hexagonal icon pattern 594, but it applies equally well to any other usable pattern symmetry. In a manner similar to the method of Fig. 23, this method relies on using different information in at least one icon area. In the example of Fig. 24A, each of two different icon patterns 596 and 598 are in half of the icon area (only one of each pattern is shown in this figure for clarity). These icon images generate a composite composite image 600 including a composite image 602 generated by the icon image element 596 and a composite image 604 generated by the icon image element 598. The two composite images 602, 604 are designed to have overlapping areas 606, 608 that appear to have 100% color depth, while the non-overlapping area 605 has a 50% color depth. The minimum dimension of the overlapped region in the composite composite image may be as small as the composite magnified-scaled positioning accuracy of the icon image element, and thus may be smaller than the minimum feature size of two constituent composite images designed to overlap in the small region. . In the example of Fig. 23, the overlapping area is used to generate a character of the number " 10 " which is otherwise narrower than possible.

This method can also be used to create a narrow gap pattern between icon picture elements as shown in Fig. 24B. Hexagon icon area 609 may be square or any other suitable shape to make a space-filled array, but hexagons are preferred. In this example, half of the icon pattern is icon image 610 and half is icon image 611. Ideally these two patterns would be distributed relatively uniformly between the icon regions. In isolation these two patterns do not clearly indicate the shape of the final image, which can be used as a security element-the image is not apparent until it is formed by an overlapping lens array. An example of a composite image 612 is shown that is formed by a combination of a composite image of the icon element 610 and a composite image of the icon element 611, whereby the gap left between the individual composite images is a number "10". To form. In this case, the two composite images are combined to form the final composite image, so the colored portion of this image 613 shows 50% color density. This method is not limited by the details of this example; Three icons may be used instead of the two, and the gaps forming certain elements in the composite composite image may have a variable width and non-limiting shape diversity, which is the method of Fig. 23, Fig. 24A, B, or Fig. 25. Or in combination with other icon image design methods taught by the applicant.

The icon image may contain covertly hidden information not found in the resulting composite image. Such covert information hidden in the icon picture can be used, for example, for covert authentication of an object. Two ways to accomplish this are shown in FIG. The first method is illustrated by the use of matching icon images 616, 618. Icon image 616 shows a solid boundary pattern and the number " 42 " contained within the boundary. Icon image 618 shows a solid shape having the number " 42 " as a graphic hole therein. In this example, the periphery shapes of the icon images 616 and 618 are almost identical, and their relative positions within their respective icon areas 634 and 636 are also substantially the same. When the composite composite image 620 is generated from these icon images, the boundary of the composite composite image 622 will show 100% color density because all icon images have a pattern in their corresponding area, and thus the icon image 616, The composite image generated from 618 is completely superimposed. Since the image of the space surrounding "42" comes from the icon image 618 that fills only half of the icon area and the colored "42" image also comes from the icon image 616 that fills half of the icon image, the composite composite image ( The color depth of the interior 624 of 620 will be 50%. As a result, there is no hue difference between "42" and its background, so the composite composite image 626 that is observed will represent an image with a 100% color depth boundary 628 and a 50% color depth interior 630. The "42" secretly present throughout the iconic images 616 and 618 is therefore "neutralized" and will not be visible in the observed composite composite image 626.

A second method of including covert information in the icon image is shown by triangle 632 in FIG. The triangle 632 may be randomly placed in the icon area (not shown in this figure) or may be arranged in an array or other pattern that does not substantially match the period of the icon area 634, 632. A composite image is generated from a plurality of regularly arranged icon images picked up by corresponding regular micro-lens arrays. Patterns in the icon plane that hardly coincide with the period of the micro-lens array will not form a complete composite image. Thus, the pattern of triangles 632 will not produce a consistent composite image and will not be visible in the observed composite image 626. This method is not limited to simple geometric designs such as triangle 632, and other covert information such as alphanumeric information, bar codes, data bits, and large-scale patterns can be included in the icon plane in this way.

Figure 26 illustrates a general method for generating a full three-dimensional integrated image in unison material. The single icon area 640 includes an icon image 642 showing a scale-deformed view of the object to be displayed in three dimensions when viewed at an advantageous point in this icon area 640. In this case, the icon image 642 is designed to form a composite image 670 of the hollow cube 674. Icon image 642 is a foreground frame 644 representing the closest side 674 of the hollow cube 672, and a tapered gap pattern 646 representing the corner 676 of the hollow cube 672. And a background frame 648 representing the furthest side 678 of the hollow cube 672. Note that the relative ratio of the foreground frame 644 to the background frame 648 in the icon image 642 does not match the ratio of the closest side 674 and the furthest side 678 of the composite image hollow cube 672. Able to know. The reason for the scale difference is that an image looking farther away from the plane of unison material undergoes greater magnification, and therefore its size within the icon image must be reduced to provide accurate scale upon magnification to form composite image 672. Because.

At different locations on the Unison 3-D material, an icon region 650 is found with a different icon image 652. Like icon image 642, icon image 652 represents a scale-modified view of composite image 672 when viewed at another advantageous point in this icon area 650. The relative scaling of the foreground frame 654 and the background frame 658 is similar to (or generally not true to) the corresponding elements of the icon image 642, but the position of the background frame 658 is the size of the corner pattern 656. And moved with orientation. The icon area 660 is located further on the Unison 3-D material, which is another scale-modified icon image with a foreground frame 664, a tapered gap pattern 667, and a background frame 668. 662).

In general, the icon picture in each icon area in Unison 3-D material may be slightly different from its nearest neighbor and significantly different from its far neighbor. It can be seen that icon image 652 represents the transition stage between icon images 642 and 662. In general, each icon area in Unison 3-D material may be unique, but each angle will represent a transition stage between icon pictures to either side.

The composite image 670 is formed of a number of icon images, such as icon images 640, 650, 660 that are symmetrically picked up through an associated lens array. The composite image of the hollow cube 674 shows the effect of different composite magnification factors due to the effective repetition period of the different elements of each of the icon images. It is assumed that hollow cube image 674 is intended to be observed as a superdeep image. In this case, when the icon region 640 is disposed at a distance from the lower left of the icon region 650 and the icon region 660 is disposed at a distance from the upper right portion of the icon region 650, the foreground frames 644 and 654. 664 will be shorter than the valid period of background frames 648, 658, 668, so that the closest face 676 of the cube (corresponding to foreground frames 644, 654, 664) is unison It can be seen that the surface located closer to the plane of material and the furthest face 678 of the cube is located farther from the plane of unison material and is enlarged by a large factor. Corner elements 646, 656, 667 cooperate with the foreground element and the background element to create a smoothly varying depth effect therebetween.

The icon image design method for Unison 3-D is described more fully in FIG. This figure isolates the method for a single image projector 680. As mentioned above, a single image projector has a lens, an optical spacer, and an icon image, the icon image having approximately the same dimensions as the repetition period of the lens (allowing a small scale difference to produce a union visual effect). The field of view of the lens and its associated icon is shown as cone 682, which also corresponds to the inverse of the focal cone of the lens, so the ratio of the field of view cone 682 is determined by the F # of the lens. Although the cone is shown as having a circular base, the base shape will be substantially the same as the shape of the icon area, such as a hexagon.

In this example, we want to create a Unison 3-D composite image that contains three copies 686, 690, 694 of the word "UNISON" at the same visual size in three different superdeep image planes 684, 688, 692. do. The diameter of the image planes 684, 688, 692 expands with the viewing cone, i.e. as the image depth increases, the area covered by the viewing cone increases. Thus, the field of view in the shallowest depth plane 684 includes only the "NIS" portion of the word UNISON, while the intermediate depth plane 688 includes the entirety of "NIS" and portions of "U" and "O", The deep depth plane 692 covers almost the entirety of "UNISON" and only part of the last "N" is missing.

The information (UNISONs 686, 690, 694) provided by each of these composite image planes 684, 688, 692 should ultimately be included in a single icon image in image projector 680. This is accomplished by capturing information on the viewing cone 686 at each depth plane 684, 688, 692 and then scaling the resulting icon image pattern to the same dimensions. Icon image 696 represents the field of view of the UNISON image 686 viewed from the depth plane 684, icon image 704 represents the field of view of the UNISON image 690 viewed from the depth plane 688, and icon image 716. Denotes a field of view of the UNISON image 694 as viewed from the depth plane 692.

In the icon picture 696, the icon picture element 698 starts at the part of the first "N" of the UNISON picture 686, and the icon picture element 700 is at the part of "I" of the UNISON picture 686. And the icon picture element 702 starts at the portion of "S" of the UNISON picture 686. Within the icon picture 704, the icon picture element 706 starts at a portion of the "U" of the UNISON picture 690, and the icon picture element 708 starts at the first "N" of the UNISON picture 690, Icon picture element 710 starts at "S" in UNISON picture 690 and icon picture element 714 starts at part of "O" in UNISON picture 690. It should be noted that the composite images 686, 690, 694 are provided on a similar scale, but the icon image 704 in the medium depth plane 688 represents its UNISON letters on a smaller scale than that of the icon image 696. . This will cause the icon image 704 to experience a higher composite magnification (when combined with multiple surrounding icon images in the same depth plane). Similarly, the icon image 716 includes an icon image element 718 originating in the UNISON image 694, and the UNISON characters included in the icon image are further scaled down.

The final icon image in this image projector is generated by combining these three icon images 696, 704 and 716 into the single icon image 730 shown in FIG. The combined icon element 732 includes all the graphic information and depth information needed for the image projector 680 to contribute to the composite image formed from the multiple image projectors, each of which has its own centered on the image projector. Specific icon image information resulting from the intersection of the field of view cone and the level and elements of the composite image to be generated. Since each image projector is displaced by at least one lens repetition period from all other image projectors, each image projector will have different information due to the intersection of its viewing cone and the composite image space.

Each of the icon images required to represent the selected 3-D image is obtained by knowing the three-dimensional digital model of the composite image, the predetermined depth position and depth span to be provided to the composite image, the lens repetition period, the lens field of view, and the ultimate graphic resolution of the icon image. Can be calculated. The last factor places an upper limit on the level of detail that can be provided in each depth plane. Since the depth plane, which lies further away from the plane of unison material, has a large amount of information (due to field of view increase), the graphical resolution limit of the icon has the greatest effect on the resolution of these composite image depth planes.

FIG. 29 shows how the method of FIG. 27 can be applied to complex three-dimensional composite images, such as the image of "the Lady of Brassempouy" 742, which is a valuable ice age giant ivory carving craft. An individual image projector 738, including at least a lens, optical spacing element, and icon image (not shown in this figure) lies in a plane 740 of unison material that separates the float composite image space from the deep composite image space. . In this example, the composite image space spans the Unison material so that a portion of the image is placed in the float composite image space and a portion is in the deep composite image space. Image projector 738 has an almost conical view extending into deep composite image space 744 and float composite image space 746. A predetermined number of deep image planes 748 and 752-762 are selected depending on how much space is needed to obtain the desired deep composite image spatial resolution. Similarly, a predetermined number of float image planes 750 and 764-774 are selected depending on how much space is needed to obtain the desired float composite image spatial resolution. Some of these planes, for example dip plane 748 and float plane 750, will extend beyond the composite image and will not contribute to the final information in the icon image. For clarity, the number of image planes shown in FIG. 29 is limited to a small number, but the actual number of image planes selected may be as large as possible to achieve the desired composite image depth resolution, for example, 50 to 100 or more. Can be.

The method of FIGS. 27 and 28 is then applied to obtain an icon image in each depth plane by determining the intersection shape of the surface of the object 742 and the selected depth planes 756-774. The resulting individual icon picture is scaled to the final size of the combined icon picture. The entire float icon image is first rotated 180 degrees (returns to its exact orientation in the composite image as it will undergo its rotation again when projected) and then the dip icon to form the final icon image for this image projector 738. Combined with the image. This process is repeated so that each position of the image projector obtains a complete pattern of icon images necessary to form the entire composite image 742.

The resolution of the composite image depends on the resolution of the optical projector and the graphic resolution of the icon image. Icon image graphic resolutions of less than 0.1 micron were obtained that exceeded the theoretical optical resolution limit of 0.2 microns. Typical icon images are created at a resolution of 0.25 microns.

Unison materials may be manufactured by sheet or web processing using tools that include lenses and icon microstructures separately. Lens tools and icon tools are started using photo mask and photoresist methods.

The lens tool is initially designed as a semiconductor mask, usually a black chrome on glass. Masks with sufficient resolution may be produced by photoreduction, electron beam writing, or laser writing. Conventional lens tool masks will include a repeating opaque hexagonal pattern of selected periods, such as 30 microns, with the hexagons separated by clear lines less than 2 microns wide. This mask is then used to expose the photoresist on the glass plate using a conventional semiconductor UV exposure system. The thickness of the resist is selected to obtain the desired deflection of the lens. For example, a 5 micron thick AZ 4620 positive on a glass plate by suitable means such as spin coating, dip coating, meniscus coating, or spraying to form a lens having a nominal 30 micron repeat and a nominal 35 micron focal length. The photoresist is coated. The photoresist is exposed in a mask pattern, developed on glass in a conventional manner, and then dried and degassed at 100 ° C. for 30 minutes. The lens is formed by thermal reflow according to standard methods known in the art. The resulting photoresist micro-lens is coated with a conductive metal such as gold or silver, and the negative nickel tool is produced by electroforming.

Icon tools are created in a similar way. Icon patterns are typically designed with the aid of CAD software, which is then passed on to the semiconductor mask manufacturer. This mask is used in a similar manner to a lens mask except that the thickness to be exposed of the resist is usually 0.5 micron to 8 microns, depending on the optical density of the desired composite image. The photoresist is exposed in a mask pattern, developed on glass in a conventional manner, then coated with a conductive metal, and a negative nickel tool is produced by electroplating. Depending on the choice of the original mask design and also in the selection of the resist form (positive or negative) used, the icon can be created in the form of a void in the resist pattern, or in the form of a "mesa" or post in the resist pattern or both. Can be generated.

Unison materials can be made from a variety of materials and various methods known in the micro-optical and microstructure replication arts, including extrusion embossing, radiation cured casting, soft embossing, injection molding, reaction co-injection molding, and reactive casting. An exemplary manufacturing method forms an icon as a void in a radiation cured liquid polymer that is cast against a base film, such as a 75 gauge adhesion-promoting PET film, and then the lens is placed in the correct alignment to the icon or obliquely opposite the base film. Formed into a radiation cured polymer, followed by filling the icon voids with submicron particle coloring coloring material by gravure-type doctor blading to the film surface, and filling the fill with suitable means (e.g. solvent removal, radiation curing, or chemical reaction). ), To apply an optional sealing layer which may be finally clear, colored, dyed or comprising a secret security material.

The manufacture of the unison motion material requires that the icon tool and the lens tool have a selected degree of misalignment of the two arrays of symmetry axes. This misalignment of the icon and lens pattern symmetry axis controls the composite image size and composite image rotation in the material produced. It is sometimes desirable to provide a composite image that is nearly aligned with the web direction or the cross-web direction, in which case the overall angular misalignment of the icon and the lens is equally divided between the lens pattern and the icon pattern. The degree of angular misalignment required is typically quite small. For example, a 0.3 degree overall angular misalignment is suitable to enlarge a 30 micron icon image to a size of 5.7 mm in unison motion material. In this example, the overall angular misalignment is equally divided between the two tools, so that each tool is inclined over an angle of 0.15 degrees in the same direction for both tools. These inclinations are in the same direction because the tools form microstructures on opposite sides of the base film, so the inclinations of the tools are added to each other instead of canceling each other out.

The inclination can be provided to the tool in the initial design of the mask by rotating the desired angle before recording the entire pattern. Inclination can also be provided mechanically on flat nickel tools, which can be provided by cutting the tool at an appropriate angle with a numerically controlled milling machine. The inclined tool is then formed into a cylindrical tool using inclined-cutting edges to align with the axis of rotation of the impression cylinder.

Synthetic magnified micro-optical systems herein include, for example, inks, metals, fluorescent or magnetic materials, X-rays, infrared or ultraviolet absorbing or emissive materials, magnetics including aluminum, nickel, chromium, silver, gold and Positive or negative materials, including but not limited to non-magnetic metals, laminated or coated inks with aqueous, solvent or radiation curable, optically clear, translucent or opaque, colored or dyed indices in the form of coatings or prints, and / or Or an icon fill material, back coating, top coating, patterned and unpatterned fill or inclusion in a lens, optical spacer or icon material as an adhesive; Magnetic coatings and particles for detection or storage of information; Fluorescent dyes and pigments as coatings and particles; IR fluorescent coatings, fillers, dyes or particles; UV fluorescent coatings, fillers, dyes or particles; Coatings and particles, planchettes, DNA, RNA, or other macro-molecule taggants, dichroic fibers, radioisotopes, print receptive coatings, sizing, or primers, chemically reactive materials, micro- Encapsulating components, magnetic field-affecting materials, metallic and nonmetallic conductive particles and coatings, microperforated holes, colored silver wire or fibers, on surfaces of documents, labels or materials that are bonded as carriers to paper or polymer to adhere to the paper during manufacture Patches, fluorescent dichroic silver wires or particles of embedded, raman scattering coatings or particles, color shifting coatings or particles, unisons, silver wires laminated on paper, cardboard, cardboard, plastic, ceramic, textile or metal substrates, Unison as a patch, label, overlap, hot stamp foil or tear tape, holographic, refractive kinegram, isogram, photo With a graphical or refractive optical elements, liquid crystal materials, Up Conversion and Down Conversion materials as a single element or a variety of combinations can be combined with additional features that are not limited to these examples.

Synthetic augmented micro-optical systems herein have a variety of uses and applications, examples of which include:

Government and defense uses-whether in federal, state or foreign affairs (e.g. passports, ID cards, driver's licenses, visas, birth certificates, vital records, voter registration cards, ballot papers, security cards, bonds, foodstuffs) Distribution rights, stamps, and tax recognition);

Currency-whether in federal, state or foreign affairs (eg, hidden lines in paper money, features in polymer money, and features on paper money);

Documents (eg, titles, date certificates, licenses, diplomas, and certificates);

Financial and distribution tools (eg, certified bank checks, household checks, bank slips, sovereignty, traveler's checks, money orders, credit cards, debit cards, ATM cards, affiliate cards, prepaid phone cards, and gift cards);

Confidential information (eg, screenplays, legal documents, intellectual property, medical records / hospital records, prescription forms / pads);

Product and brand protection, including Fabric & Home Care (eg, laundry detergents, softeners, dish detergents, household detergents, surface coatings, garment deodorants, bleaches, specialty material care);

Cosmetic care (eg, hair care, hair color, skin care and cleansing, cosmetics, perfumes, antiperspirants, deodorants, protective pads for women, tampons, and pantyliners);

Infant and household care (eg, baby diapers, baby and infant towels, baby bibs, baby change and bed mats, paper towels, toilet paper, and facial tissues);

Healthcare (e.g., oral care, pet health and nutrition, prescription drugs, retail drugs, drug delivery and personal health care, prescription vitamins, and sports and nutritional supplements; prescription and over-the-counter eyeglasses; hospitals, healthcare professionals, and wholesale healthcare Medical devices and equipment sold to vendors, ie bandages, devices, embedded devices, surgical instruments);

Food and beverage packaging;

Textile packaging;

Electronic devices, parts and assemblies;

Apparel and footwear, including sportswear, footwear, licensed and unlicensed luxury, sports and luxury apparel, textiles;

Biotech drugs;

Aerospace components and components;

Automotive components and parts;

Sporting goods;

Tobacco products;

software;

CDs and DVDs;

gunpowder;

New items (eg, gift wrap and ribbons);

Books and magazines;

School supplies and office supplies;

Business card;

Shipping documentation and packaging;

Note cover;

Book cover;

Bookmark;

Event and transport tickets;

Gambling and gaming uses (eg, lottery tickets, game cards, casino chips, and items for use in casinos, lottery sales and betting games);

Home furniture (eg, towels, linens, and furniture);

Flooring and wallpaper;

Jewelry and watches;

handbag;

Art, collectibles and souvenirs;

toy;

Displays (eg point of sale information management and promotional displays);

Product marking and labeling (e.g., labels, labels, tags, strings, tear strips, over-wraps, tamper proof applied as camouflage and asset tracking to branded products or documents for certification or promotion) Burn protection).

Suitable materials for the foregoing embodiments include a wide range of polymers. Acrylics, acrylated polyesters, acrylated urethanes, polypropylenes, epoxies, urethanes, and polyesters have suitable optical and mechanical properties for both microlenses and microstructured icon elements. Suitable materials for optional substrate films include most of the commercially available polymer films including acrylics, cellophane, sarans, nylons, polycarbonates, polyesters, polypropylenes, polyethylenes, and polyvinyls. The microstructured icon filling material may comprise any of the materials described above as suitable for preparing microstructured icon elements as well as solvent based inks and other commonly available dye or pigment vehicles. The dyes or pigments included in these materials should be compatible with the chemical structure of the medium. The pigment should have a particle size substantially smaller than the minimum dimension of any component of the icon element. The optional seal layer material is one of the materials described above as suitable for making microstructure icon elements, as well as a variety of other commercially available paints, inks, overcoats, varnishes, lacquers, and clear coats used in the printing and paper and film converting industries. Any may be provided. There is no preferred combination of materials, and the choice of materials depends on the detail of the material shape, the optical properties of the system, and the desired optical effects.

While exemplary embodiments have been disclosed and described, those skilled in the art will recognize that there may be many variations, modifications or variations of the invention described above. In all such variations, modifications and variations are therefore to be understood as included within the scope of the present invention.

Claims (84)

(a) one or more optical spacers, (b) a micro-image composed of a periodic planar array of a plurality of image icons having an axis of symmetry about at least one of the plane axes, disposed on or adjacent to the optical spacer, and (c) a composite magnification micro-optical system comprising a periodic planar array of image icon focusing elements having an axis of symmetry about at least one of the plane axes, the axis of symmetry being the same plane axis as that of the micro image plane array, each focusing element Is an aspherical focusing element with an effective diameter of less than 50 microns, the focal length is the shortest in vertical observation and increases with angle of inclination, Wherein each focusing element is a polygonal base multi-domain lens. The group of claim 1 wherein the focusing element is a group consisting of a circular base, a hexagonal base, a rounded hexagonal base, a square base, a triangular base, a rounded triangular base, and a mixed base thereof in the plane of its planar array. Synthetic magnification micro-optical system having a base shape selected from. The composite magnification micro-optic system of claim 1, wherein the focusing element has an F number of 4 or less. 3. The composite magnification micro-optic system of claim 2, wherein the focusing element has an F number of 4 or less. The synthesized magnification microcomputer according to claim 1, wherein the scaling ratio of the repetition period of the picture icon to the repetition period of the focusing element is equal to 1, and the axis of symmetry of the periodic planar array of the micro picture and the periodic planar array of the picture icon focusing element is misaligned. -Optical system. 6. The composite magnification micro-optic system of claim 5, wherein quadrature motion effects are provided. The synthesized magnification microcomputer according to claim 1, wherein the scaling ratio of the repetition period of the picture icon to the repetition period of the focusing element is greater than 1, and the axis of symmetry of the periodic planar array of the micro picture and the periodic planar array of the picture icon focusing element is aligned. -Optical system. The composite magnification micro- of claim 1, wherein the scaling ratio of the repetition period of the picture icon to the repetition period of the focusing element is less than 1, and the axis of symmetry of the periodic planar array of the micro picture and the periodic planar array of the picture icon focusing element is aligned. Optical system. The scaling factor of claim 1, wherein the scaling ratio of the repetition period of the image icon to the repetition period of the focusing element is axially asymmetric in the plane of the image icon and the focusing element, the scaling ratio being less than 1 in one axis of symmetry and the other axis of symmetry. Is greater than 1 and wherein the axis of symmetry of the periodic planar array of micro-pictures and the periodic planar array of image-icon focusing elements is aligned. The composite magnifying micro-optical system of claim 1, wherein each focusing element has an effective diameter of 15 to 30 microns. The composite magnifying micro-optic system of claim 1, wherein each focusing element has an effective diameter of less than 30 microns. The composite magnified micro-optic system of claim 1, having an overall thickness of less than 45 microns. The synthetic magnification micro-optic system of claim 1, having an overall thickness of 10 to 40 microns. The composite magnification micro-optic system of claim 1, wherein each focusing element has a focal length of less than 40 microns. The composite magnification micro-optic system of claim 1, wherein each focusing element has a focal length of less than 10 to 30 microns. The composite magnification micro-optic system of claim 1, wherein a morphing effect is provided for morphing one composite magnified image into another composite magnified image. The composite magnification micro-optical system of claim 1, wherein each image icon is formed by a printing method selected from the group consisting of inkjet, laserjet, letterpress, flexo, gravure, and intaglio printing methods. The composite magnification micro-optic system of claim 1, wherein the picture icon is formed as a recess in the substrate, and voids in the recess are filled with evaporated metal material, dyeing material, coloring material, and combinations thereof. 2. The system of claim 1, comprising two picture icon layers at different depths in the system, wherein some of the combination of focusing elements has a focal length for focusing on one picture icon layer of one of the two picture icon layers; Is a composite zoom micro-optical system having a focal length for focusing on different image icon layers. 2. The composite magnification micro-optic system of claim 1, wherein the focusing element is a non-cylindrical lens and a reflective layer is disposed on the side opposite the focusing element of the micro image. The composite magnification micro-optical system of claim 1 having a transparent tamper resistant material disposed over the focusing element. The composite magnification micro-optic system of claim 1, comprising a second periodic planar array of focusing elements disposed on a side opposite the focusing element of a micro picture. 23. The composite magnification micro-optic system of claim 22, comprising a second planar array of picture icons between two planar arrays of focusing elements. A document security device comprising a composite magnification micro-optical system according to any one of claims 1 to 23. (a) providing one or more optical spacers, (b) providing a micro image consisting of a periodic planar array of a plurality of image icons having an axis of symmetry about at least one of the plane axes, disposed on or adjacent to the optical spacer, and (c) providing a periodic planar array of image icon focusing elements having an axis of symmetry about at least one of the plane axes, wherein the axis of symmetry is the same plane as that of the micro image plane array. Axis, each focusing element is an aspherical focusing element having an effective diameter of less than 50 microns and associated with an image icon, the focal length being the shortest in vertical observation and increasing as the angle of view increases, Wherein each focusing element is a polygonal base multi-domain lens. A method of manufacturing a document security device comprising the steps (a), (b) and (c) of claim 25. 27. The group comprising steps (a), (b) and (c) of claim 25, wherein the scaling ratio of the repetition period of the picture icon to the repetition period of the focusing element is less than one, equal to one, and greater than one Selecting and selecting whether the axis of symmetry of the periodic planar array of micropictures and the axis of symmetry of the periodic planar array of image icon focusing elements are aligned or misaligned. 27. The group comprising steps (a), (b) and (c) of claim 25, wherein the scaling ratio of the repetition period of the picture icon to the repetition period of the focusing element is less than one, equal to one, and greater than one And selecting whether the axis of symmetry of the periodic planar array of micropictures and the axis of symmetry of the periodic planar array of image icon focusing elements are aligned or misaligned. delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete delete

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